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Prof.Dr. İbrahim USLU | Gazi University - Academia.edu

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class="left-panel-container"><div class="user-info-component-wrapper"><div class="user-summary-cta-container"><div class="user-summary-container"><div class="social-profile-avatar-container"><img class="profile-avatar u-positionAbsolute" alt="Prof.Dr. İbrahim USLU" border="0" onerror="if (this.src != &#39;//a.academia-assets.com/images/s200_no_pic.png&#39;) this.src = &#39;//a.academia-assets.com/images/s200_no_pic.png&#39;;" width="200" height="200" src="https://0.academia-photos.com/820891/285303/337453/s200__brahim.uslu.jpg" /></div><div class="title-container"><h1 class="ds2-5-heading-sans-serif-sm">Prof.Dr. İbrahim USLU</h1><div class="affiliations-container fake-truncate js-profile-affiliations"><div><a class="u-tcGrayDarker" href="https://gazi.academia.edu/">Gazi University</a>, <a class="u-tcGrayDarker" href="https://gazi.academia.edu/Departments/Chemistry_Education/Documents">Chemistry Education</a>, <span class="u-tcGrayDarker">Faculty 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class="stat-container js-profile-followees" data-broccoli-component="user-info.followees-count" data-click-track="profile-expand-user-info-following"><p class="label">Following</p><p class="data">2,163</p></div></a><a><div class="stat-container js-profile-coauthors" data-broccoli-component="user-info.coauthors-count" data-click-track="profile-expand-user-info-coauthors"><p class="label">Co-authors</p><p class="data">10</p></div></a><a href="https://gazi.academia.edu/ibrahimUSLU/Analytics"><div class="stat-container"><p class="label"><span class="js-profile-total-view-text">Public Views</span></p><p class="data"><span class="js-profile-view-count"></span></p></div></a></div><div class="user-bio-container"><div class="profile-bio fake-truncate js-profile-about" style="margin: 0px;">I am a Prof.Dr. at Gazi University, mainly working on nanotechnolgy, life sciences. Phytotherapy is also my professional area. I have some trade marks for ex. Candiex, Fitoderman, Lauradenti, Geniwash. www.fitoderman.com is the internet site you can find these products. You can find my papers at https://scholar.google.com.tr/citations?user=1RHseU0AAAAJ<br /><span class="u-fw700">Phone:&nbsp;</span>0312 202 1928<br /><b>Address:&nbsp;</b>Gazi University<br />Eğitim Fakültesi<br />Teknik Okullar Beşevler<br />Ankara TURKEY<br /><div class="js-profile-less-about u-linkUnstyled u-tcGrayDarker u-textDecorationUnderline u-displayNone">less</div></div></div><div class="ri-section"><div class="ri-section-header"><span>Interests</span><a class="ri-more-link js-profile-ri-list-card" data-click-track="profile-user-info-primary-research-interest" data-has-card-for-ri-list="820891">View All (24)</a></div><div class="ri-tags-container"><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="820891" href="https://www.academia.edu/Documents/in/Materials_Science_and_Engineering"><div id="js-react-on-rails-context" style="display:none" data-rails-context="{&quot;inMailer&quot;:false,&quot;i18nLocale&quot;:&quot;en&quot;,&quot;i18nDefaultLocale&quot;:&quot;en&quot;,&quot;href&quot;:&quot;https://gazi.academia.edu/ibrahimUSLU&quot;,&quot;location&quot;:&quot;/ibrahimUSLU&quot;,&quot;scheme&quot;:&quot;https&quot;,&quot;host&quot;:&quot;gazi.academia.edu&quot;,&quot;port&quot;:null,&quot;pathname&quot;:&quot;/ibrahimUSLU&quot;,&quot;search&quot;:null,&quot;httpAcceptLanguage&quot;:null,&quot;serverSide&quot;:false}"></div> <div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{&quot;color&quot;:&quot;gray&quot;,&quot;children&quot;:[&quot;Materials Science and Engineering&quot;]}" data-trace="false" data-dom-id="Pill-react-component-2427be71-8fd0-414b-bd55-6986767ea980"></div> <div id="Pill-react-component-2427be71-8fd0-414b-bd55-6986767ea980"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="820891" href="https://www.academia.edu/Documents/in/Nanotechnology"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{&quot;color&quot;:&quot;gray&quot;,&quot;children&quot;:[&quot;Nanotechnology&quot;]}" data-trace="false" data-dom-id="Pill-react-component-0ae5a173-1fc0-4f20-a9df-eb8266076fec"></div> <div id="Pill-react-component-0ae5a173-1fc0-4f20-a9df-eb8266076fec"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="820891" href="https://www.academia.edu/Documents/in/Biotechnology"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{&quot;color&quot;:&quot;gray&quot;,&quot;children&quot;:[&quot;Biotechnology&quot;]}" data-trace="false" data-dom-id="Pill-react-component-56d082e0-5b0e-4fdc-b6f1-5392977e6f7b"></div> <div id="Pill-react-component-56d082e0-5b0e-4fdc-b6f1-5392977e6f7b"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="820891" href="https://www.academia.edu/Documents/in/Chemistry_Education"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{&quot;color&quot;:&quot;gray&quot;,&quot;children&quot;:[&quot;Chemistry Education&quot;]}" data-trace="false" data-dom-id="Pill-react-component-932f7152-ae33-4f61-a6da-e9b5bea29a15"></div> <div id="Pill-react-component-932f7152-ae33-4f61-a6da-e9b5bea29a15"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="820891" href="https://www.academia.edu/Documents/in/Nuclear_Engineering"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{&quot;color&quot;:&quot;gray&quot;,&quot;children&quot;:[&quot;Nuclear Engineering&quot;]}" data-trace="false" data-dom-id="Pill-react-component-8e4ff97b-92e8-4504-8e8b-c36d439f4d21"></div> <div id="Pill-react-component-8e4ff97b-92e8-4504-8e8b-c36d439f4d21"></div> </a></div></div><div class="external-links-container"><ul class="profile-links new-profile js-UserInfo-social"><li class="left-most js-UserInfo-social-cv" data-broccoli-component="user-info.cv-button" data-click-track="profile-user-info-cv" data-cv-filename="ozgecmis_ing.doc" data-placement="top" data-toggle="tooltip" href="/ibrahimUSLU/CurriculumVitae"><button class="ds2-5-text-link ds2-5-text-link--small" style="font-size: 20px; 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The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuing exposure, and health impacts to a static local population for a 1000-year period following the end of disposal operations. Human exposure scenarios include normal releases (including leaching and operational spillage), human intrusion, and limited site farming or reclamation. Pathways and processes of transport from the trench to an individual or population include ground-water transport, overland flow, erosion, surface water dilution, suspension, atmospheric transport and deposition, inhalation, external exposure, and ingestion of contaminated beef, milk, crops, and water. The proposed waste disposal area in Koteyli, Balikesir, Turkey, has been evaluated using the PRESTO-II methodol...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0bba5375257f18f66287f5ceaef24d7f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234150,&quot;asset_id&quot;:67405743,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234150/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405743"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405743"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405743; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405743]").text(description); $(".js-view-count[data-work-id=67405743]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405743; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405743']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405743, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "0bba5375257f18f66287f5ceaef24d7f" } } $('.js-work-strip[data-work-id=67405743]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405743,"title":"Evaluation of proposed shallow-land burial sites using the PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) methodology and code","translated_title":"","metadata":{"abstract":"PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) is a computer code designed to evaluate possible doses and risks (health effects) from shallow-land burial sites. 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The Turkish ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The Turkish government is in the process of planning two nuclear reactors in Turkey. The Turkish Atomic Energy Authority has been given the task of developing plans for improved control of low-level wastes (LLW) in Turkey. Principal sources of radioactive wastes are hospitals, research institutions, biological research centers, universities, industries, and two research reactors in Turkey. These wastes will be treated in a pilot water treatment facility located in Cekmece Nuclear Research and Training Center, Istanbul. In this temporary waste disposal facility, the wastes will be stored in 200-l concrete containers until the establishment of the permanent waste disposal sites in Turkey in 1990. The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405740"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405740"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405740; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405740]").text(description); $(".js-view-count[data-work-id=67405740]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405740; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405740']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405740, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405740]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405740,"title":"Studies involving proposed waste disposal facilities in Turkey","translated_title":"","metadata":{"abstract":"The Turkish government is in the process of planning two nuclear reactors in Turkey. 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The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...","publication_date":{"day":null,"month":null,"year":1987,"errors":{}},"publication_name":"Transactions of the American Nuclear Society"},"translated_abstract":"The Turkish government is in the process of planning two nuclear reactors in Turkey. The Turkish Atomic Energy Authority has been given the task of developing plans for improved control of low-level wastes (LLW) in Turkey. Principal sources of radioactive wastes are hospitals, research institutions, biological research centers, universities, industries, and two research reactors in Turkey. These wastes will be treated in a pilot water treatment facility located in Cekmece Nuclear Research and Training Center, Istanbul. In this temporary waste disposal facility, the wastes will be stored in 200-l concrete containers until the establishment of the permanent waste disposal sites in Turkey in 1990. The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...","internal_url":"https://www.academia.edu/67405740/Studies_involving_proposed_waste_disposal_facilities_in_Turkey","translated_internal_url":"","created_at":"2022-01-06T09:56:50.489-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Studies_involving_proposed_waste_disposal_facilities_in_Turkey","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"The Turkish government is in the process of planning two nuclear reactors in Turkey. The Turkish Atomic Energy Authority has been given the task of developing plans for improved control of low-level wastes (LLW) in Turkey. Principal sources of radioactive wastes are hospitals, research institutions, biological research centers, universities, industries, and two research reactors in Turkey. These wastes will be treated in a pilot water treatment facility located in Cekmece Nuclear Research and Training Center, Istanbul. In this temporary waste disposal facility, the wastes will be stored in 200-l concrete containers until the establishment of the permanent waste disposal sites in Turkey in 1990. The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405738"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405738/Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders"><img alt="Research paper thumbnail of Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405738/Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders">Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders</a></div><div class="wp-workCard_item"><span>Materials Chemistry and Physics</span><span>, 2012</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel techni...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405738"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405738"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405738; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405738]").text(description); $(".js-view-count[data-work-id=67405738]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405738; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405738']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405738, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405738]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405738,"title":"Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders","translated_title":"","metadata":{"abstract":"A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...","publication_date":{"day":null,"month":null,"year":2012,"errors":{}},"publication_name":"Materials Chemistry and Physics"},"translated_abstract":"A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...","internal_url":"https://www.academia.edu/67405738/Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders","translated_internal_url":"","created_at":"2022-01-06T09:56:50.394-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405734"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405734/Radyasyon_kaynaklar%C4%B1_ve_etkileri"><img alt="Research paper thumbnail of Radyasyon kaynakları ve etkileri" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405734/Radyasyon_kaynaklar%C4%B1_ve_etkileri">Radyasyon kaynakları ve etkileri</a></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405734"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405734"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405734; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405733"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey"><img alt="Research paper thumbnail of Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey">Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the c...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405733"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405733"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405733; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405733]").text(description); $(".js-view-count[data-work-id=67405733]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405733; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405733']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405733, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405733]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405733,"title":"Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey","translated_title":"","metadata":{"abstract":"Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...","publication_date":{"day":null,"month":null,"year":1988,"errors":{}}},"translated_abstract":"Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...","internal_url":"https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey","translated_internal_url":"","created_at":"2022-01-06T09:56:50.146-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405731"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes"><img alt="Research paper thumbnail of PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes" class="work-thumbnail" src="https://attachments.academia-assets.com/78234047/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes">PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. This site selection was based partially on the need to consider a variety of hydrologic and climatic situations, and partially on the availability of data. The results obtained for the operational low-level waste disposal site at Barnwell, South Carolina, are presented for comparison. 6 refs., 2 figs., 1 tab.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b7731c4c2e2a622ab574f6810a5b6d77" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234047,&quot;asset_id&quot;:67405731,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234047/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405731"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405731"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405731; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405731]").text(description); $(".js-view-count[data-work-id=67405731]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405731; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405731']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405731, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b7731c4c2e2a622ab574f6810a5b6d77" } } $('.js-work-strip[data-work-id=67405731]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405731,"title":"PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes","translated_title":"","metadata":{"abstract":"The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. 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The results obtained for the operational low-level waste disposal site at Barnwell, South Carolina, are presented for comparison. 6 refs., 2 figs., 1 tab.","internal_url":"https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes","translated_internal_url":"","created_at":"2022-01-06T09:56:50.023-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":78234047,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234047/thumbnails/1.jpg","file_name":"5816080.pdf","download_url":"https://www.academia.edu/attachments/78234047/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"PRESTO_II_computer_code_for_safety_asses.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234047/5816080-libre.pdf?1641531070=\u0026response-content-disposition=attachment%3B+filename%3DPRESTO_II_computer_code_for_safety_asses.pdf\u0026Expires=1733898196\u0026Signature=K88T8GqQCwl9jRVKUI9~2wFXzdHKltDbYpl38BKsuuRhay7cVQ3DmN5s9OaXScLoGrQOEZTNtkk1QLXNFE1ev05v5LVmGqgi2AHjGRbRFBO6AR8JSugxN2zsf4~HgDCSChbWuX8BZnrVoIBTvx3gJoZ18V6amC~ep3FCcaHMRalR-9AgUa3eZ-G901JcnaxqSyzFSrCEcPTRqp2ybpHHmrKOVmQU2GfEnHMVBsYPC5nAAxjKV-0cPqCxrpDlmlrvFUfVTTIc2XUaN9jE7RJUh-WqwfGTA8wumSm13DgUYBFjPWwPlGGoVii5uxbLI~7kRd-y6xB-zn57AZn0JXQdRw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes","translated_slug":"","page_count":5,"language":"en","content_type":"Work","summary":"The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. This site selection was based partially on the need to consider a variety of hydrologic and climatic situations, and partially on the availability of data. 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Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405729"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405729"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405729; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405729]").text(description); $(".js-view-count[data-work-id=67405729]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405729; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405729']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405729, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405729]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405729,"title":"Synthesis and characterization of boron-doped bismuth oxide-erbium oxide fiber derived nanocomposite precursor","translated_title":"","metadata":{"abstract":"In this study, boron doped and undoped Bi2O3-Er2O3 nanocomposite fibers were produced via electrospinning technique. Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...","publication_date":{"day":null,"month":null,"year":2014,"errors":{}}},"translated_abstract":"In this study, boron doped and undoped Bi2O3-Er2O3 nanocomposite fibers were produced via electrospinning technique. Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...","internal_url":"https://www.academia.edu/67405729/Synthesis_and_characterization_of_boron_doped_bismuth_oxide_erbium_oxide_fiber_derived_nanocomposite_precursor","translated_internal_url":"","created_at":"2022-01-06T09:56:49.905-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Synthesis_and_characterization_of_boron_doped_bismuth_oxide_erbium_oxide_fiber_derived_nanocomposite_precursor","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405728"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal"><img alt="Research paper thumbnail of High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal">High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electros...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405728"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405728"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405728; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405728]").text(description); $(".js-view-count[data-work-id=67405728]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405728; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405728']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405728, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405728]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405728,"title":"High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal","translated_title":"","metadata":{"abstract":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","publication_date":{"day":null,"month":null,"year":2015,"errors":{}}},"translated_abstract":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","internal_url":"https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal","translated_internal_url":"","created_at":"2022-01-06T09:56:49.777-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles"},{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":4496,"name":"Composites","url":"https://www.academia.edu/Documents/in/Composites"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":66399,"name":"Synthesis and Characterization of nanomaterials","url":"https://www.academia.edu/Documents/in/Synthesis_and_Characterization_of_nanomaterials"},{"id":91080,"name":"Nano Technology","url":"https://www.academia.edu/Documents/in/Nano_Technology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":106128,"name":"Thermoelectric Materials","url":"https://www.academia.edu/Documents/in/Thermoelectric_Materials"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405727"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers"><img alt="Research paper thumbnail of Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers" class="work-thumbnail" src="https://attachments.academia-assets.com/78234045/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers">Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="93166baa8c793b5090b2127cc4cbbd9e" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234045,&quot;asset_id&quot;:67405727,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405727"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405727"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405727; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405727]").text(description); $(".js-view-count[data-work-id=67405727]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405727; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405727']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405727, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "93166baa8c793b5090b2127cc4cbbd9e" } } $('.js-work-strip[data-work-id=67405727]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405727,"title":"Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers","translated_title":"","metadata":{"abstract":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","publication_date":{"day":null,"month":null,"year":2009,"errors":{}}},"translated_abstract":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. 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Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","internal_url":"https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers","translated_internal_url":"","created_at":"2022-01-06T09:56:49.587-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":78234045,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234045/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234045/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=YBA5YLU2Qv1wIEmF3zMYvMwXeT2yU5DGtECjcxoylTUMxJZx2Vl8Oq8WpaYv8NjlIqXfdQh938o5IpD6YH4zdhfJsSYrqAzx8bVvIPUfJLPEAylJtgS67PiBcJnRIo6eqsbd9QDN53Jp-itH7H7YDcResQcqThQH8ElFOTibg7HNE2NmBVQ4bqDxxQFSjQOfIa2pdDIz5LbpivojTsXQ5xK3iwrwt7FaE4-30b1guCr9U2maj4NhTqhm6cG-zPg9GRvVlZD~7j8iY8ADl7wcSSghyRz~3aFu3sy9HFdbDv5PRVMAcP2tskZEig3smmYOupYZEjZ3bnM-8DPpWvCN5A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers","translated_slug":"","page_count":5,"language":"en","content_type":"Work","summary":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":78234045,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234045/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234045/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=YBA5YLU2Qv1wIEmF3zMYvMwXeT2yU5DGtECjcxoylTUMxJZx2Vl8Oq8WpaYv8NjlIqXfdQh938o5IpD6YH4zdhfJsSYrqAzx8bVvIPUfJLPEAylJtgS67PiBcJnRIo6eqsbd9QDN53Jp-itH7H7YDcResQcqThQH8ElFOTibg7HNE2NmBVQ4bqDxxQFSjQOfIa2pdDIz5LbpivojTsXQ5xK3iwrwt7FaE4-30b1guCr9U2maj4NhTqhm6cG-zPg9GRvVlZD~7j8iY8ADl7wcSSghyRz~3aFu3sy9HFdbDv5PRVMAcP2tskZEig3smmYOupYZEjZ3bnM-8DPpWvCN5A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":78234046,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234046/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234046/download_file","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234046/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=Bsf1ccXGAynsGZv-dJhLDqrZ90hV0FEb7p3Zc2KNVAnvOkOZ~m03x9uvzx2YL4uxzCCg7zrBc2PlP8Yo8gPrHwXV4ud2~68TVjbueI4YKJZWSdmxca-hBl~Pmoc2LN3gp-6Dq-6SngEFtUvRqRqLUr8FyC4401IPSu33H4N8sVRbp4JRQAKvWqTvUZu5lrmbCd72kiVihAO6QAGAMpWyKwqB-lFsC6FchyHtCMx3ue9Pj7eBuFnHuDO0f0xcQqPJuiiGsQPYC~9V2A69oswzwCaGkPmb69wOi7iAafvWNCGdosr7TDejU3yx4fhzGb3jOEqn3rScIQfMT7IS34i2eg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":7871,"name":"FTIR spectroscopy","url":"https://www.academia.edu/Documents/in/FTIR_spectroscopy"},{"id":8702,"name":"Nanofabrication","url":"https://www.academia.edu/Documents/in/Nanofabrication"},{"id":12010,"name":"Electrospinning","url":"https://www.academia.edu/Documents/in/Electrospinning"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":23992,"name":"Nanochemistry","url":"https://www.academia.edu/Documents/in/Nanochemistry"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":56396,"name":"PVA","url":"https://www.academia.edu/Documents/in/PVA"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":139262,"name":"DSC","url":"https://www.academia.edu/Documents/in/DSC"},{"id":139272,"name":"Crosslinking","url":"https://www.academia.edu/Documents/in/Crosslinking"},{"id":186923,"name":"Co","url":"https://www.academia.edu/Documents/in/Co"},{"id":358523,"name":"Electrospun fiber","url":"https://www.academia.edu/Documents/in/Electrospun_fiber"},{"id":386261,"name":"Boron doped cobalt","url":"https://www.academia.edu/Documents/in/Boron_doped_cobalt"},{"id":389192,"name":"Amorphous","url":"https://www.academia.edu/Documents/in/Amorphous"},{"id":389193,"name":"Amorphous Structure","url":"https://www.academia.edu/Documents/in/Amorphous_Structure"},{"id":389195,"name":"Fourpoint","url":"https://www.academia.edu/Documents/in/Fourpoint"},{"id":389196,"name":"Fourpoint Probe","url":"https://www.academia.edu/Documents/in/Fourpoint_Probe"},{"id":389832,"name":"Poly Vinyl Alcohol","url":"https://www.academia.edu/Documents/in/Poly_Vinyl_Alcohol"}],"urls":[{"id":16170304,"url":"http://www.hjbc.hacettepe.edu.tr/site/assets/files/2944/37_3_227-231.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405726"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405726/Preparation_and_Characterization_of_Polyvinyl_Alcohol_Based_Copolymers_as_Wound_Dressing_Fibers"><img alt="Research paper thumbnail of Preparation and Characterization of Polyvinyl Alcohol Based Copolymers as Wound Dressing Fibers" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405726/Preparation_and_Characterization_of_Polyvinyl_Alcohol_Based_Copolymers_as_Wound_Dressing_Fibers">Preparation and Characterization of Polyvinyl Alcohol Based Copolymers as Wound Dressing Fibers</a></div><div class="wp-workCard_item"><span>International Journal of Polymeric Materials</span><span>, Jul 23, 2015</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405726"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405726"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405726; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405587"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer"><img alt="Research paper thumbnail of Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O&lt;italic&gt;x&lt;/italic&gt;) Interlayer" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer">Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O&lt;italic&gt;x&lt;/italic&gt;) Interlayer</a></div><div class="wp-workCard_item"><span>IEEE Transactions on Electron Devices</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectr...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${C}/{G}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\text {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) and resistance (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{i}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\varepsilon ^\prime $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;, &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\varepsilon ^{\prime \prime }$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;), electric modulus (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${M}^\prime $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${M}^{\prime \prime }$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;), and ac conductivity (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\sigma _{\mathsf {ac}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) were calculated from the &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${C}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${G}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;. The observed peaks in the &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{i}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; plots can be ascribed by the special distribution of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;CO&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;Ga&amp;lt;sub&amp;gt;0.001&amp;lt;/sub&amp;gt;O&amp;lt;sub&amp;gt;&amp;lt;italic&amp;gt;x&amp;lt;/italic&amp;gt;&amp;lt;/sub&amp;gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and series resistance (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{s}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;). The values of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\sigma $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405587"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405587"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405587; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405587]").text(description); $(".js-view-count[data-work-id=67405587]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405587; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405587']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405587, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405587]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405587,"title":"Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O\u003citalic\u003ex\u003c/italic\u003e) Interlayer","translated_title":"","metadata":{"abstract":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","publisher":"Institute of Electrical and Electronics Engineers (IEEE)","publication_name":"IEEE Transactions on Electron Devices"},"translated_abstract":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","internal_url":"https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer","translated_internal_url":"","created_at":"2022-01-06T09:55:59.344-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":1237788,"name":"Electrical And Electronic Engineering","url":"https://www.academia.edu/Documents/in/Electrical_And_Electronic_Engineering"}],"urls":[{"id":16170238,"url":"http://xplorestaging.ieee.org/ielx7/16/8440584/08425996.pdf?arnumber=8425996"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="60792622"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/60792622/Investigation_of_the_effect_of_different_Bi2O3_x_PVA_x_Sm_Sn_Mo_thin_insulator_interface_layer_materials_on_diode_parameters"><img alt="Research paper thumbnail of Investigation of the effect of different Bi2O3–x:PVA (x = Sm, Sn, Mo) thin insulator interface-layer materials on diode parameters" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/60792622/Investigation_of_the_effect_of_different_Bi2O3_x_PVA_x_Sm_Sn_Mo_thin_insulator_interface_layer_materials_on_diode_parameters">Investigation of the effect of different Bi2O3–x:PVA (x = Sm, Sn, Mo) thin insulator interface-layer materials on diode parameters</a></div><div class="wp-workCard_item"><span>Journal of Materials Science: Materials in Electronics</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="60792622"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="60792622"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 60792622; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="42683169"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders"><img alt="Research paper thumbnail of CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders" class="work-thumbnail" src="https://attachments.academia-assets.com/62892827/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders">CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/%C3%B6zgeg%C3%B6kmen">özge gökmen</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://gazi.academia.edu/ibrahimUSLU">Prof.Dr. İbrahim USLU</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="d2a442f95e5e5e5a97071e965f30c7b1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:62892827,&quot;asset_id&quot;:42683169,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/62892827/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="42683169"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="42683169"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 42683169; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=42683169]").text(description); $(".js-view-count[data-work-id=42683169]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 42683169; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='42683169']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 42683169, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "d2a442f95e5e5e5a97071e965f30c7b1" } } $('.js-work-strip[data-work-id=42683169]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":42683169,"title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders","translated_title":"","metadata":{"abstract":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.","publication_date":{"day":null,"month":null,"year":2013,"errors":{}}},"translated_abstract":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.","internal_url":"https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders","translated_internal_url":"","created_at":"2020-04-09T16:25:33.957-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":48920836,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":34170036,"work_id":42683169,"tagging_user_id":48920836,"tagged_user_id":48920836,"co_author_invite_id":7008069,"email":"g***e@gmail.com","display_order":1,"name":"özge gökmen","title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders"},{"id":34170037,"work_id":42683169,"tagging_user_id":48920836,"tagged_user_id":820891,"co_author_invite_id":null,"email":"p***u@gmail.com","affiliation":"Gazi University","display_order":2,"name":"Prof.Dr. İbrahim USLU","title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders"}],"downloadable_attachments":[{"id":62892827,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/62892827/thumbnails/1.jpg","file_name":"Ceramics_Intrenational_201320200409-103310-lrnn4v.pdf","download_url":"https://www.academia.edu/attachments/62892827/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"CERAMICS_INTERNATIONAL_Structural_invest.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/62892827/Ceramics_Intrenational_201320200409-103310-lrnn4v-libre.pdf?1586475341=\u0026response-content-disposition=attachment%3B+filename%3DCERAMICS_INTERNATIONAL_Structural_invest.pdf\u0026Expires=1733898196\u0026Signature=JeTtiiugpdmaVaPOikdZzfGyHuS7AxZapGzqwNFH7CLKzgcrzhrRXU0-wGbR1H-HWCdqSfBvOhhxxeLIbnV1LndUAasON4NwyfVcTn7I4~j4Gyygsn5DGXOirYW5BeGuUTvkNruKibjczn-qreg9rUPXB6PFYrakdpkKM77oPyTpqP6rK1R~G9FLoH9hOi9kW7Dr3eGZi47seB-kL3VoGvPR7uH8716Lvv7ZLorRKWIVr9FyDZpF3NsjRQAjX6OYYOAmVGzmYrU9wvQJ1z0ns250EIVO2GVBeh~XV7nJXkvVbSrSNBh6kQOIGC~fEWMvAKjDsmyK5rert1hxA3fojA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders","translated_slug":"","page_count":6,"language":"en","content_type":"Work","summary":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. 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The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="341e74b2252352fbf4d5ed18a0176e9b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671641,&quot;asset_id&quot;:36729583,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729583"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729583"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729583; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729583]").text(description); $(".js-view-count[data-work-id=36729583]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729583; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729583']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729583, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "341e74b2252352fbf4d5ed18a0176e9b" } } $('.js-work-strip[data-work-id=36729583]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729583,"title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods","translated_title":"","metadata":{"doi":"10.1007/s12034-018-1602-6","volume":"41","abstract":"Three different thicknesses (50, 150 and 500 nm) Zn-doped polyvinyl alcohol (PVA) was deposited on n-4H-SiC wafer as interlayer by electrospinning method and so, Au/(Zn-doped PVA)/n-4H-SiC metal–polymer–semiconductor structures were fabricated. The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.","page_numbers":"82","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Bulletin of Materials Science"},"translated_abstract":"Three different thicknesses (50, 150 and 500 nm) Zn-doped polyvinyl alcohol (PVA) was deposited on n-4H-SiC wafer as interlayer by electrospinning method and so, Au/(Zn-doped PVA)/n-4H-SiC metal–polymer–semiconductor structures were fabricated. The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.","internal_url":"https://www.academia.edu/36729583/A_comparative_study_on_dielectric_behaviours_of_Au_Zn_doped_PVA_n_4H_SiC_MPS_structures_with_different_interlayer_thicknesses_using_impedance_spectroscopy_methods","translated_internal_url":"","created_at":"2018-05-28T03:06:58.280-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470282,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":6684049,"email":"f***r@sdu.edu.tr","display_order":1,"name":"Ahmet Faruk Özdemir","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470283,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":46531121,"co_author_invite_id":null,"email":"a***l@gazi.edu.tr","display_order":2,"name":"Ş. Altındal","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470284,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":6684050,"email":"v***n@gmail.com","display_order":3,"name":"H. E. Lapa","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470285,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":4,"name":"A. Kökçe","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"}],"downloadable_attachments":[{"id":56671641,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671641/thumbnails/1.jpg","file_name":"10.1004.pdf","download_url":"https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_comparative_study_on_dielectric_behavi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671641/10.1004-libre.pdf?1527502376=\u0026response-content-disposition=attachment%3B+filename%3DA_comparative_study_on_dielectric_behavi.pdf\u0026Expires=1733355286\u0026Signature=MjAf1DZdf4pw99sZ1Dze5Esuf15SYtUEDSnlnaHI-8HxzXa8fkSkQAtmlcE1shMywx8vEz3LeQwQs02ByUXNFkZUiphasMaMReMu4M~ColYdNzJqywb1llbBmGDzM54giGzccvGXXQTir3AjAtKeh-O2YGdLvXUvAMmQmLGw3iti3GucRrdMBQnkv0zUYFTrj2xbwJ52hrr4HMPFDG7TLdKTVbbANCFowUBdYgdPfyEtoCdoC6jeUUr2k8Bga-CheNMixUgoJaNSRzUOnuiFOo3eQRhUsfy1IBs2H6T-rgw-ZVrBl9tPAsa~l8U~JAXBagwQBZxrWM1OwKqeiJ9TRQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"A_comparative_study_on_dielectric_behaviours_of_Au_Zn_doped_PVA_n_4H_SiC_MPS_structures_with_different_interlayer_thicknesses_using_impedance_spectroscopy_methods","translated_slug":"","page_count":6,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU","email":"RUVNbEhsVGZqdC94MFVUQnRLQi9oRkNzVndRdUJyNWgxdkd3aWtIRHlGdnhSUVhUQ1RHSmNteDJCT1lsUmYwVi0tNU8wb2kxOHluNm5uelVvcTdKQTVhUT09--02f3c170f13bb37b6d7a70ab31c01b8d2863d08c"},"attachments":[{"id":56671641,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671641/thumbnails/1.jpg","file_name":"10.1004.pdf","download_url":"https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_comparative_study_on_dielectric_behavi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671641/10.1004-libre.pdf?1527502376=\u0026response-content-disposition=attachment%3B+filename%3DA_comparative_study_on_dielectric_behavi.pdf\u0026Expires=1733355286\u0026Signature=MjAf1DZdf4pw99sZ1Dze5Esuf15SYtUEDSnlnaHI-8HxzXa8fkSkQAtmlcE1shMywx8vEz3LeQwQs02ByUXNFkZUiphasMaMReMu4M~ColYdNzJqywb1llbBmGDzM54giGzccvGXXQTir3AjAtKeh-O2YGdLvXUvAMmQmLGw3iti3GucRrdMBQnkv0zUYFTrj2xbwJ52hrr4HMPFDG7TLdKTVbbANCFowUBdYgdPfyEtoCdoC6jeUUr2k8Bga-CheNMixUgoJaNSRzUOnuiFOo3eQRhUsfy1IBs2H6T-rgw-ZVrBl9tPAsa~l8U~JAXBagwQBZxrWM1OwKqeiJ9TRQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering"},{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":519,"name":"Solid State Physics","url":"https://www.academia.edu/Documents/in/Solid_State_Physics"},{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":532,"name":"Physical Chemistry","url":"https://www.academia.edu/Documents/in/Physical_Chemistry"},{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles"},{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":23992,"name":"Nanochemistry","url":"https://www.academia.edu/Documents/in/Nanochemistry"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":66399,"name":"Synthesis and Characterization of nanomaterials","url":"https://www.academia.edu/Documents/in/Synthesis_and_Characterization_of_nanomaterials"},{"id":91080,"name":"Nano Technology","url":"https://www.academia.edu/Documents/in/Nano_Technology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":1019454,"name":"Nano Fabrication","url":"https://www.academia.edu/Documents/in/Nano_Fabrication"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729558"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures"><img alt="Research paper thumbnail of Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures" class="work-thumbnail" src="https://attachments.academia-assets.com/56671613/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures">Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures</a></div><div class="wp-workCard_item"><span>Journal of Electronic Materials</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) s...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63436e5bb95fa4027fc62470378091d9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671613,&quot;asset_id&quot;:36729558,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671613/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729558"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729558"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729558; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729558]").text(description); $(".js-view-count[data-work-id=36729558]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729558; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729558']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729558, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "63436e5bb95fa4027fc62470378091d9" } } $('.js-work-strip[data-work-id=36729558]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729558,"title":"Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures","translated_title":"","metadata":{"doi":"10.1007/s11664-018-6195-8","abstract":"The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Journal of Electronic Materials"},"translated_abstract":"The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.","internal_url":"https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures","translated_internal_url":"","created_at":"2018-05-28T03:00:43.625-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470255,"work_id":36729558,"tagging_user_id":820891,"tagged_user_id":1303640,"co_author_invite_id":null,"email":"b***f@gmail.com","affiliation":"İstanbul Ticaret Üniversitesi","display_order":1,"name":"Yosef badali","title":"Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures"},{"id":31470256,"work_id":36729558,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":3,"name":"A. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729519"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure"><img alt="Research paper thumbnail of On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure" class="work-thumbnail" src="https://attachments.academia-assets.com/56671568/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure">On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure</a></div><div class="wp-workCard_item"><span>Journal of Materials Science: Materials in Electronics</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="fef1eda6f8eed5bba58e59f896acd832" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671568,&quot;asset_id&quot;:36729519,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671568/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729519; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729519]").text(description); $(".js-view-count[data-work-id=36729519]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729519; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729519']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729519, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "fef1eda6f8eed5bba58e59f896acd832" } } $('.js-work-strip[data-work-id=36729519]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729519,"title":"On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure","translated_title":"","metadata":{"doi":"10.1007/s10854-017-8219-1","volume":"29","abstract":"The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","page_numbers":"2890-2898","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Journal of Materials Science: Materials in Electronics"},"translated_abstract":"The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","internal_url":"https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure","translated_internal_url":"","created_at":"2018-05-28T02:52:30.827-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470237,"work_id":36729519,"tagging_user_id":820891,"tagged_user_id":46531121,"co_author_invite_id":null,"email":"a***l@gazi.edu.tr","display_order":1,"name":"Ş. Altındal","title":"On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure"},{"id":31470238,"work_id":36729519,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":3,"name":"E. E. 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Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":56671568,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671568/thumbnails/1.jpg","file_name":"on_the_ana.pdf","download_url":"https://www.academia.edu/attachments/56671568/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"On_the_anomalous_peak_and_negative_capac.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671568/on_the_ana-libre.pdf?1527501526=\u0026response-content-disposition=attachment%3B+filename%3DOn_the_anomalous_peak_and_negative_capac.pdf\u0026Expires=1733756524\u0026Signature=drVeJNG3fDWtBqg3DGDExLK6OixBhfnMMVMslIE54tnfjfct7kiafbYhJB1-TALyG7XMPDjnYfIUE-DAOUjBcA6mO~cmsKKBVZulxM0I3NKeQEslPSJyztE7Lw9d9gNEsGh-53cyHwcn6pMlYCQYNdXhOkvTlt1q37fMg1bQj-~I2JALya9~hcBY0cqNGkICVcLYgksP-j~DY~g2SZv35aL3jlw86pvz3jIlfJFFqXEsNnJeKp6Y3SWvhP-F0VqsWK9y2DvxT76vlrZZEOVcTHatrlHzBQQUhitIG1-g0ioRu9IBqgxRzDsvzzp4a22y95lvoCcDC48~rf6J1W4Axw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":144046,"name":"Frequency","url":"https://www.academia.edu/Documents/in/Frequency"},{"id":389165,"name":"Voltage","url":"https://www.academia.edu/Documents/in/Voltage"}],"urls":[{"id":8509618,"url":"https://link.springer.com/article/10.1007%2Fs10854-017-8219-1"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729474"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729474/Thermoelectric_Properties_of_nickel_and_boron_co_substituted_Prepared_by_Electrospinning_Technique"><img alt="Research paper thumbnail of Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique" class="work-thumbnail" src="https://attachments.academia-assets.com/56671526/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729474/Thermoelectric_Properties_of_nickel_and_boron_co_substituted_Prepared_by_Electrospinning_Technique">Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique</a></div><div class="wp-workCard_item"><span> Nano Hybrids and Composites</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic p...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic powders were synthesized using electrospinning techniques and then consolidated into bulk ceramics. The differences in the microstructure and thermoelectric properties of the samples as a result of doping effect have been investigated. The crystalline structures of the powders and nanofibers were characterized using X-ray diffraction and scanning electron microscopy and BET Analysis before and after the calcination process at different temperatures. Nanofibers prepared by the use of electrospinning technique, have a diameter of approximately 300 nm, and the diameter of the grains of calcined powders was observed to range between 150 to 500 nanometers. Thermoelectric properties of the bulk ceramics were measured by physical properties measurement system (Lot-Oriel PPMS) in a temperature range of 15–300 K. The calculated values of dimensionless figure of merit at 300 K are , , and for sintered powders from undoped, Ni and B doped powders, respectively.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="117c5104cbaee706f452fcfeaf238939" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671526,&quot;asset_id&quot;:36729474,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671526/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729474"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729474"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729474; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729474]").text(description); $(".js-view-count[data-work-id=36729474]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729474; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729474']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729474, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "117c5104cbaee706f452fcfeaf238939" } } $('.js-work-strip[data-work-id=36729474]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729474,"title":"Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique","translated_title":"","metadata":{"doi":"10.4028/www.scientific.net/NHC.19.34","volume":"19","abstract":"In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic powders were synthesized using electrospinning techniques and then consolidated into bulk ceramics. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="39712" id="papers"><div class="js-work-strip profile--work_container" data-work-id="67405743"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405743/Evaluation_of_proposed_shallow_land_burial_sites_using_the_PRESTO_II_Prediction_of_Radiation_Effects_from_Shallow_Trench_Operations_methodology_and_code"><img alt="Research paper thumbnail of Evaluation of proposed shallow-land burial sites using the PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) methodology and code" class="work-thumbnail" src="https://attachments.academia-assets.com/78234150/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405743/Evaluation_of_proposed_shallow_land_burial_sites_using_the_PRESTO_II_Prediction_of_Radiation_Effects_from_Shallow_Trench_Operations_methodology_and_code">Evaluation of proposed shallow-land burial sites using the PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) methodology and code</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) is a computer code des...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) is a computer code designed to evaluate possible doses and risks (health effects) from shallow-land burial sites. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuing exposure, and health impacts to a static local population for a 1000-year period following the end of disposal operations. Human exposure scenarios include normal releases (including leaching and operational spillage), human intrusion, and limited site farming or reclamation. Pathways and processes of transport from the trench to an individual or population include ground-water transport, overland flow, erosion, surface water dilution, suspension, atmospheric transport and deposition, inhalation, external exposure, and ingestion of contaminated beef, milk, crops, and water. The proposed waste disposal area in Koteyli, Balikesir, Turkey, has been evaluated using the PRESTO-II methodol...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0bba5375257f18f66287f5ceaef24d7f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234150,&quot;asset_id&quot;:67405743,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234150/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405743"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405743"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405743; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405743]").text(description); $(".js-view-count[data-work-id=67405743]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405743; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405743']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405743, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "0bba5375257f18f66287f5ceaef24d7f" } } $('.js-work-strip[data-work-id=67405743]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405743,"title":"Evaluation of proposed shallow-land burial sites using the PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) methodology and code","translated_title":"","metadata":{"abstract":"PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) is a computer code designed to evaluate possible doses and risks (health effects) from shallow-land burial sites. 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The Turkish ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The Turkish government is in the process of planning two nuclear reactors in Turkey. The Turkish Atomic Energy Authority has been given the task of developing plans for improved control of low-level wastes (LLW) in Turkey. Principal sources of radioactive wastes are hospitals, research institutions, biological research centers, universities, industries, and two research reactors in Turkey. These wastes will be treated in a pilot water treatment facility located in Cekmece Nuclear Research and Training Center, Istanbul. In this temporary waste disposal facility, the wastes will be stored in 200-l concrete containers until the establishment of the permanent waste disposal sites in Turkey in 1990. The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405740"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405740"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405740; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405740]").text(description); $(".js-view-count[data-work-id=67405740]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405740; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405740']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405740, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405740]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405740,"title":"Studies involving proposed waste disposal facilities in Turkey","translated_title":"","metadata":{"abstract":"The Turkish government is in the process of planning two nuclear reactors in Turkey. 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The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...","internal_url":"https://www.academia.edu/67405740/Studies_involving_proposed_waste_disposal_facilities_in_Turkey","translated_internal_url":"","created_at":"2022-01-06T09:56:50.489-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Studies_involving_proposed_waste_disposal_facilities_in_Turkey","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"The Turkish government is in the process of planning two nuclear reactors in Turkey. The Turkish Atomic Energy Authority has been given the task of developing plans for improved control of low-level wastes (LLW) in Turkey. Principal sources of radioactive wastes are hospitals, research institutions, biological research centers, universities, industries, and two research reactors in Turkey. These wastes will be treated in a pilot water treatment facility located in Cekmece Nuclear Research and Training Center, Istanbul. In this temporary waste disposal facility, the wastes will be stored in 200-l concrete containers until the establishment of the permanent waste disposal sites in Turkey in 1990. The PRESTO-II (prediction of radiation effects from shallow trench operations) computer code has been applied for the general probable sites for LLW disposal in Turkey. The model is intended to serve as a non-site-specific screening model for assessing radionuclide transport, ensuring exposur...","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405738"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405738/Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders"><img alt="Research paper thumbnail of Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405738/Crystal_structure_and_electrical_properties_of_gadolinia_doped_bismuth_oxide_nanoceramic_powders">Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders</a></div><div class="wp-workCard_item"><span>Materials Chemistry and Physics</span><span>, 2012</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel techni...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405738"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405738"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405738; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405738]").text(description); $(".js-view-count[data-work-id=67405738]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405738; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405738']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405738, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405738]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405738,"title":"Crystal structure and electrical properties of gadolinia doped bismuth oxide nanoceramic powders","translated_title":"","metadata":{"abstract":"A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...","publication_date":{"day":null,"month":null,"year":2012,"errors":{}},"publication_name":"Materials Chemistry and Physics"},"translated_abstract":"A novel method of fabrication of gadolinia doped bismuth oxide nanoceramic via the sol–gel technique is reported. Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. 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Their thermal, structural and morphological properties are described by measurements of Differential Thermal Analysis/Thermal Gravimetry, X-ray Powder Diffraction and Scanning Electron Microscopy. The samples have stable high ion conductive face centered cubic δ-phase nanocrystalline structure. The electrical measurements of the nanoceramic powders were carried out in the temperature range of (689–1091 K) using 4-point probe technique. There is a transition between two distinct regions at 720 °C, which can be attributed to the order–disorder transition. This observation is supported by the differential thermal analysis measurements. The experimental results show that the value of conductivity increases with increasing temperature over linear parts characterized by two different activation energies. The conductivity data over whole measured temperature range were fitted t...","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405736"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405736/Discharge_policies_for_low_level_radioactive_effluents_in_Turkey"><img alt="Research paper thumbnail of Discharge policies for low level radioactive effluents in Turkey" class="work-thumbnail" src="https://attachments.academia-assets.com/78234149/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405736/Discharge_policies_for_low_level_radioactive_effluents_in_Turkey">Discharge policies for low level radioactive effluents in Turkey</a></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="508575b7d97105ce1bf0f1e69e366cd5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234149,&quot;asset_id&quot;:67405736,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234149/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405736"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405736"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405736; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405733"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey"><img alt="Research paper thumbnail of Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey">Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the c...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405733"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405733"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405733; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405733]").text(description); $(".js-view-count[data-work-id=67405733]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405733; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405733']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405733, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405733]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405733,"title":"Correlation between thorium concentrations in soil and gamma readings in FUSRAP site in New Jersey","translated_title":"","metadata":{"abstract":"Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...","publication_date":{"day":null,"month":null,"year":1988,"errors":{}}},"translated_abstract":"Thorium ores were processed in Wayne and Maywood, New Jersey, between 1916 and 1956. During the course of Th processing, the wastes from the operations were pumped into dikes next to the plant. Construction in the area caused the dispersal of waste into adjacent areas. The Department of Energy (DOE) adopted a policy of assigning an independent verification contractor to ensure the effectiveness of remedial action performed within the Formerly Utilized Sites Remedial Action Program (FUSRAP). The Environmental assessment group of Oak Ridge National Laboratory was assigned the responsibility for this task at the Maywood and Wayne, New Jersey sites. The soil samples collected from the area were analyzed to determine the thorium concentration. In this study, a correlation is described between the thorium concentration and the gamma readings of the site. The statistical analysis of the data indicates that this correlation is site-specific and depends on the depth of the radionuclide. Data...","internal_url":"https://www.academia.edu/67405733/Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey","translated_internal_url":"","created_at":"2022-01-06T09:56:50.146-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Correlation_between_thorium_concentrations_in_soil_and_gamma_readings_in_FUSRAP_site_in_New_Jersey","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405731"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes"><img alt="Research paper thumbnail of PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes" class="work-thumbnail" src="https://attachments.academia-assets.com/78234047/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes">PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. This site selection was based partially on the need to consider a variety of hydrologic and climatic situations, and partially on the availability of data. The results obtained for the operational low-level waste disposal site at Barnwell, South Carolina, are presented for comparison. 6 refs., 2 figs., 1 tab.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b7731c4c2e2a622ab574f6810a5b6d77" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234047,&quot;asset_id&quot;:67405731,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234047/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405731"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405731"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405731; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405731]").text(description); $(".js-view-count[data-work-id=67405731]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405731; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405731']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405731, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b7731c4c2e2a622ab574f6810a5b6d77" } } $('.js-work-strip[data-work-id=67405731]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405731,"title":"PRESTO-II computer code for safety assessment on shallow land disposal of low-level wastes","translated_title":"","metadata":{"abstract":"The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. 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The results obtained for the operational low-level waste disposal site at Barnwell, South Carolina, are presented for comparison. 6 refs., 2 figs., 1 tab.","internal_url":"https://www.academia.edu/67405731/PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes","translated_internal_url":"","created_at":"2022-01-06T09:56:50.023-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":78234047,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234047/thumbnails/1.jpg","file_name":"5816080.pdf","download_url":"https://www.academia.edu/attachments/78234047/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"PRESTO_II_computer_code_for_safety_asses.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234047/5816080-libre.pdf?1641531070=\u0026response-content-disposition=attachment%3B+filename%3DPRESTO_II_computer_code_for_safety_asses.pdf\u0026Expires=1733898196\u0026Signature=K88T8GqQCwl9jRVKUI9~2wFXzdHKltDbYpl38BKsuuRhay7cVQ3DmN5s9OaXScLoGrQOEZTNtkk1QLXNFE1ev05v5LVmGqgi2AHjGRbRFBO6AR8JSugxN2zsf4~HgDCSChbWuX8BZnrVoIBTvx3gJoZ18V6amC~ep3FCcaHMRalR-9AgUa3eZ-G901JcnaxqSyzFSrCEcPTRqp2ybpHHmrKOVmQU2GfEnHMVBsYPC5nAAxjKV-0cPqCxrpDlmlrvFUfVTTIc2XUaN9jE7RJUh-WqwfGTA8wumSm13DgUYBFjPWwPlGGoVii5uxbLI~7kRd-y6xB-zn57AZn0JXQdRw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"PRESTO_II_computer_code_for_safety_assessment_on_shallow_land_disposal_of_low_level_wastes","translated_slug":"","page_count":5,"language":"en","content_type":"Work","summary":"The PRESTO-II (Prediction of Radiation Effects from Shallow Trench Operations) computer code has been applied for the following sites; Koteyli, Balikesir and Kozakli, Nevsehir in Turkey. This site selection was based partially on the need to consider a variety of hydrologic and climatic situations, and partially on the availability of data. 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Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405729"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405729"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405729; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405729]").text(description); $(".js-view-count[data-work-id=67405729]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405729; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405729']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405729, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405729]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405729,"title":"Synthesis and characterization of boron-doped bismuth oxide-erbium oxide fiber derived nanocomposite precursor","translated_title":"","metadata":{"abstract":"In this study, boron doped and undoped Bi2O3-Er2O3 nanocomposite fibers were produced via electrospinning technique. Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...","publication_date":{"day":null,"month":null,"year":2014,"errors":{}}},"translated_abstract":"In this study, boron doped and undoped Bi2O3-Er2O3 nanocomposite fibers were produced via electrospinning technique. Obtained fibers were turned into ceramics via calcination process. Obtained nanocomposite fibers and ceramics were characterized by Fourier transform infrared, x-ray diffraction, and scanning electron microscopy techniques. X-ray diffraction results show that boron undoped Bi2O3-Er2O3 ceramic consisted of face-centered cubic Bi2O3-Er2O3 phase. However, boron doped Bi2O3-Er2O3 ceramic consisted of orthorhombic phase. Crystallite sizes of the ceramics were evaluated using Scherrer’s equation. Crystallite sizes of boron doped and undoped ceramics were calculated as 50 and 17 nm, respectively. The average fiber diameters for boron doped and undoped poly vinyl alcohol/Bi-Er acetate nanofibers were calculated as 79 nm and 96 nm, respectively. The Brunauer Emmett teller results show that boron undoped and doped Bi2O3-Er2O3 nanocrystalline powder ceramic structures sintered a...","internal_url":"https://www.academia.edu/67405729/Synthesis_and_characterization_of_boron_doped_bismuth_oxide_erbium_oxide_fiber_derived_nanocomposite_precursor","translated_internal_url":"","created_at":"2022-01-06T09:56:49.905-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Synthesis_and_characterization_of_boron_doped_bismuth_oxide_erbium_oxide_fiber_derived_nanocomposite_precursor","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405728"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal"><img alt="Research paper thumbnail of High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal">High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electros...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405728"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405728"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405728; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405728]").text(description); $(".js-view-count[data-work-id=67405728]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405728; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405728']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405728, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405728]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405728,"title":"High Thermoelectric Performance Of Unsintered NaCo2O4 Nanocrystal","translated_title":"","metadata":{"abstract":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","publication_date":{"day":null,"month":null,"year":2015,"errors":{}}},"translated_abstract":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","internal_url":"https://www.academia.edu/67405728/High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal","translated_internal_url":"","created_at":"2022-01-06T09:56:49.777-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"High_Thermoelectric_Performance_Of_Unsintered_NaCo2O4_Nanocrystal","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"Sodium cobaltite (NaCo2O4) nano crystalline thermoelectric materials were obtained using electrospinning technique. Electrospunnanofibers was calcined at 800 oC and sintered at 850 oC in open air atmopshere. We have investigated the microstructure and thermoelectric properties of the sintered and unsintered samples for analysis sintering effect. The calcined sodium cobaltite crystal structures were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Products molded by cold pressing method, and one of the pellets were sintered at 850 oC by conventional sintering, the other not subjected to the sintering process. Thermoelectric properties of the both materials were measured by PPMS system in the temperature range 10-300 K. The dimensionless figure of merit (ZT) values at 300 K is 4×10−5and 9×10−5 for sintered and unsintered samples respectively. Although conventional sintered technique increase thermoelectric power and thermal conductivity approximately % 50 but it 4-fold decreased electrical conductivity.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles"},{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":4496,"name":"Composites","url":"https://www.academia.edu/Documents/in/Composites"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":66399,"name":"Synthesis and Characterization of nanomaterials","url":"https://www.academia.edu/Documents/in/Synthesis_and_Characterization_of_nanomaterials"},{"id":91080,"name":"Nano Technology","url":"https://www.academia.edu/Documents/in/Nano_Technology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":106128,"name":"Thermoelectric Materials","url":"https://www.academia.edu/Documents/in/Thermoelectric_Materials"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405727"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers"><img alt="Research paper thumbnail of Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers" class="work-thumbnail" src="https://attachments.academia-assets.com/78234045/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers">Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="93166baa8c793b5090b2127cc4cbbd9e" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:78234045,&quot;asset_id&quot;:67405727,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405727"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405727"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405727; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405727]").text(description); $(".js-view-count[data-work-id=67405727]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405727; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405727']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405727, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "93166baa8c793b5090b2127cc4cbbd9e" } } $('.js-work-strip[data-work-id=67405727]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405727,"title":"Characterization of Boron Doped Cobalt/Zinc Acetate Composite Fibers","translated_title":"","metadata":{"abstract":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","publication_date":{"day":null,"month":null,"year":2009,"errors":{}}},"translated_abstract":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. 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Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","internal_url":"https://www.academia.edu/67405727/Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers","translated_internal_url":"","created_at":"2022-01-06T09:56:49.587-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":78234045,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234045/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234045/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=YBA5YLU2Qv1wIEmF3zMYvMwXeT2yU5DGtECjcxoylTUMxJZx2Vl8Oq8WpaYv8NjlIqXfdQh938o5IpD6YH4zdhfJsSYrqAzx8bVvIPUfJLPEAylJtgS67PiBcJnRIo6eqsbd9QDN53Jp-itH7H7YDcResQcqThQH8ElFOTibg7HNE2NmBVQ4bqDxxQFSjQOfIa2pdDIz5LbpivojTsXQ5xK3iwrwt7FaE4-30b1guCr9U2maj4NhTqhm6cG-zPg9GRvVlZD~7j8iY8ADl7wcSSghyRz~3aFu3sy9HFdbDv5PRVMAcP2tskZEig3smmYOupYZEjZ3bnM-8DPpWvCN5A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Characterization_of_Boron_Doped_Cobalt_Zinc_Acetate_Composite_Fibers","translated_slug":"","page_count":5,"language":"en","content_type":"Work","summary":"Metal oxide ceramic thin films are widely used in the electronics industry and chemical industry as electro catalyst and as selective catalysts for oxidation. In the literature the preparation of metal oxide ceramic films has been accomplished by physical vapor deposition, chemical vapor deposition and chemical solution deposition techniques. Various metal oxide fibers were obtained by high temperature calcinations. Large surface area and high aspect ratio of metal oxide fibers may have significant industrial importance especially for catalysis and filtration applications but conventional metal oxide fiber synthesis techniques of wet, dry, melt, and gel spinning, are capable of producing polymer fibers with diameters down to the micrometer range. Electrospinning is a process capable of producing polymer fibers with nanoscale diameters [1-5] .","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":78234045,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234045/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234045/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234045/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=YBA5YLU2Qv1wIEmF3zMYvMwXeT2yU5DGtECjcxoylTUMxJZx2Vl8Oq8WpaYv8NjlIqXfdQh938o5IpD6YH4zdhfJsSYrqAzx8bVvIPUfJLPEAylJtgS67PiBcJnRIo6eqsbd9QDN53Jp-itH7H7YDcResQcqThQH8ElFOTibg7HNE2NmBVQ4bqDxxQFSjQOfIa2pdDIz5LbpivojTsXQ5xK3iwrwt7FaE4-30b1guCr9U2maj4NhTqhm6cG-zPg9GRvVlZD~7j8iY8ADl7wcSSghyRz~3aFu3sy9HFdbDv5PRVMAcP2tskZEig3smmYOupYZEjZ3bnM-8DPpWvCN5A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":78234046,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/78234046/thumbnails/1.jpg","file_name":"37_3_227-231.pdf","download_url":"https://www.academia.edu/attachments/78234046/download_file","bulk_download_file_name":"Characterization_of_Boron_Doped_Cobalt_Z.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/78234046/37_3_227-231-libre.pdf?1641531067=\u0026response-content-disposition=attachment%3B+filename%3DCharacterization_of_Boron_Doped_Cobalt_Z.pdf\u0026Expires=1733756523\u0026Signature=Bsf1ccXGAynsGZv-dJhLDqrZ90hV0FEb7p3Zc2KNVAnvOkOZ~m03x9uvzx2YL4uxzCCg7zrBc2PlP8Yo8gPrHwXV4ud2~68TVjbueI4YKJZWSdmxca-hBl~Pmoc2LN3gp-6Dq-6SngEFtUvRqRqLUr8FyC4401IPSu33H4N8sVRbp4JRQAKvWqTvUZu5lrmbCd72kiVihAO6QAGAMpWyKwqB-lFsC6FchyHtCMx3ue9Pj7eBuFnHuDO0f0xcQqPJuiiGsQPYC~9V2A69oswzwCaGkPmb69wOi7iAafvWNCGdosr7TDejU3yx4fhzGb3jOEqn3rScIQfMT7IS34i2eg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":7871,"name":"FTIR spectroscopy","url":"https://www.academia.edu/Documents/in/FTIR_spectroscopy"},{"id":8702,"name":"Nanofabrication","url":"https://www.academia.edu/Documents/in/Nanofabrication"},{"id":12010,"name":"Electrospinning","url":"https://www.academia.edu/Documents/in/Electrospinning"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":23992,"name":"Nanochemistry","url":"https://www.academia.edu/Documents/in/Nanochemistry"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":56396,"name":"PVA","url":"https://www.academia.edu/Documents/in/PVA"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":139262,"name":"DSC","url":"https://www.academia.edu/Documents/in/DSC"},{"id":139272,"name":"Crosslinking","url":"https://www.academia.edu/Documents/in/Crosslinking"},{"id":186923,"name":"Co","url":"https://www.academia.edu/Documents/in/Co"},{"id":358523,"name":"Electrospun fiber","url":"https://www.academia.edu/Documents/in/Electrospun_fiber"},{"id":386261,"name":"Boron doped cobalt","url":"https://www.academia.edu/Documents/in/Boron_doped_cobalt"},{"id":389192,"name":"Amorphous","url":"https://www.academia.edu/Documents/in/Amorphous"},{"id":389193,"name":"Amorphous Structure","url":"https://www.academia.edu/Documents/in/Amorphous_Structure"},{"id":389195,"name":"Fourpoint","url":"https://www.academia.edu/Documents/in/Fourpoint"},{"id":389196,"name":"Fourpoint Probe","url":"https://www.academia.edu/Documents/in/Fourpoint_Probe"},{"id":389832,"name":"Poly Vinyl Alcohol","url":"https://www.academia.edu/Documents/in/Poly_Vinyl_Alcohol"}],"urls":[{"id":16170304,"url":"http://www.hjbc.hacettepe.edu.tr/site/assets/files/2944/37_3_227-231.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405726"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405726/Preparation_and_Characterization_of_Polyvinyl_Alcohol_Based_Copolymers_as_Wound_Dressing_Fibers"><img alt="Research paper thumbnail of Preparation and Characterization of Polyvinyl Alcohol Based Copolymers as Wound Dressing Fibers" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405726/Preparation_and_Characterization_of_Polyvinyl_Alcohol_Based_Copolymers_as_Wound_Dressing_Fibers">Preparation and Characterization of Polyvinyl Alcohol Based Copolymers as Wound Dressing Fibers</a></div><div class="wp-workCard_item"><span>International Journal of Polymeric Materials</span><span>, Jul 23, 2015</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405726"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405726"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405726; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="67405587"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer"><img alt="Research paper thumbnail of Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O&lt;italic&gt;x&lt;/italic&gt;) Interlayer" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer">Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O&lt;italic&gt;x&lt;/italic&gt;) Interlayer</a></div><div class="wp-workCard_item"><span>IEEE Transactions on Electron Devices</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectr...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${C}/{G}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\text {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) and resistance (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{i}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\varepsilon ^\prime $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;, &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\varepsilon ^{\prime \prime }$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;), electric modulus (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${M}^\prime $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${M}^{\prime \prime }$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;), and ac conductivity (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\sigma _{\mathsf {ac}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;) were calculated from the &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${C}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${G}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;. The observed peaks in the &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{i}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;–&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${V}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; plots can be ascribed by the special distribution of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;CO&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;Ga&amp;lt;sub&amp;gt;0.001&amp;lt;/sub&amp;gt;O&amp;lt;sub&amp;gt;&amp;lt;italic&amp;gt;x&amp;lt;/italic&amp;gt;&amp;lt;/sub&amp;gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${N}_{\mathsf {ss}}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; and series resistance (&amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;${R}_{s}$ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt;). The values of &amp;lt;inline-formula&amp;gt; &amp;lt;tex-math notation=&amp;quot;LaTeX&amp;quot;&amp;gt;$\sigma $ &amp;lt;/tex-math&amp;gt;&amp;lt;/inline-formula&amp;gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="67405587"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="67405587"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 67405587; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=67405587]").text(description); $(".js-view-count[data-work-id=67405587]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 67405587; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='67405587']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 67405587, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=67405587]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":67405587,"title":"Evaluation of Electric and Dielectric Properties of Metal–Semiconductor Structures With 2% GC-Doped-(Ca3Co4Ga0.001O\u003citalic\u003ex\u003c/italic\u003e) Interlayer","translated_title":"","metadata":{"abstract":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","publisher":"Institute of Electrical and Electronics Engineers (IEEE)","publication_name":"IEEE Transactions on Electron Devices"},"translated_abstract":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","internal_url":"https://www.academia.edu/67405587/Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer","translated_internal_url":"","created_at":"2022-01-06T09:55:59.344-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Evaluation_of_Electric_and_Dielectric_Properties_of_Metal_Semiconductor_Structures_With_2_GC_Doped_Ca3Co4Ga0_001O_italic_x_italic_Interlayer","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"Electrical and dielectric properties of Au/n-Si metal–semiconductor structures with high dielectric have been examined by capacitance/conductance–voltage (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}/{G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) measurements in the frequency range of 5–500 kHz at room temperature. Voltage-dependent profiles of interface states (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\text {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) and resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were extracted from the C and G data using the low–high-frequency capacitance and Nicollian–Brews methods, respectively. The real and imaginary components of the complex dielectric constant (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;, \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\varepsilon ^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), electric modulus (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^\\prime $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${M}^{\\prime \\prime }$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;), and ac conductivity (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma _{\\mathsf {ac}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;) were calculated from the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${C}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${G}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; data. All parameters have a strong relation with frequency and voltage, especially at low frequencies due to Maxwell–Wagner relaxation and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;. The observed peaks in the \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{i}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;–\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${V}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; plots can be ascribed by the special distribution of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; at M/S interface. These results confirmed that [2% graphene cobalt-doped (Ca\u0026lt;sub\u0026gt;3\u0026lt;/sub\u0026gt;CO\u0026lt;sub\u0026gt;4\u0026lt;/sub\u0026gt;Ga\u0026lt;sub\u0026gt;0.001\u0026lt;/sub\u0026gt;O\u0026lt;sub\u0026gt;\u0026lt;italic\u0026gt;x\u0026lt;/italic\u0026gt;\u0026lt;/sub\u0026gt;)] interlayer has high-dielectric constant and can be used an interlayer instead of the traditional SiO\u0026lt;sub\u0026gt;2\u0026lt;/sub\u0026gt; at M/S interface to increase their capacitance or more charges/energy storage and reduce both the values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${N}_{\\mathsf {ss}}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; and series resistance (\u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;${R}_{s}$ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt;). The values of \u0026lt;inline-formula\u0026gt; \u0026lt;tex-math notation=\u0026quot;LaTeX\u0026quot;\u0026gt;$\\sigma $ \u0026lt;/tex-math\u0026gt;\u0026lt;/inline-formula\u0026gt; are almost constant at lower–intermediate frequencies, but they start to increase at high frequencies that are corresponding to the dc and ac conductivity, respectively.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":1237788,"name":"Electrical And Electronic Engineering","url":"https://www.academia.edu/Documents/in/Electrical_And_Electronic_Engineering"}],"urls":[{"id":16170238,"url":"http://xplorestaging.ieee.org/ielx7/16/8440584/08425996.pdf?arnumber=8425996"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="60792622"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/60792622/Investigation_of_the_effect_of_different_Bi2O3_x_PVA_x_Sm_Sn_Mo_thin_insulator_interface_layer_materials_on_diode_parameters"><img alt="Research paper thumbnail of Investigation of the effect of different Bi2O3–x:PVA (x = Sm, Sn, Mo) thin insulator interface-layer materials on diode parameters" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/60792622/Investigation_of_the_effect_of_different_Bi2O3_x_PVA_x_Sm_Sn_Mo_thin_insulator_interface_layer_materials_on_diode_parameters">Investigation of the effect of different Bi2O3–x:PVA (x = Sm, Sn, Mo) thin insulator interface-layer materials on diode parameters</a></div><div class="wp-workCard_item"><span>Journal of Materials Science: Materials in Electronics</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="60792622"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="60792622"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 60792622; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="42683169"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders"><img alt="Research paper thumbnail of CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders" class="work-thumbnail" src="https://attachments.academia-assets.com/62892827/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders">CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/%C3%B6zgeg%C3%B6kmen">özge gökmen</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://gazi.academia.edu/ibrahimUSLU">Prof.Dr. İbrahim USLU</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="d2a442f95e5e5e5a97071e965f30c7b1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:62892827,&quot;asset_id&quot;:42683169,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/62892827/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="42683169"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="42683169"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 42683169; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=42683169]").text(description); $(".js-view-count[data-work-id=42683169]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 42683169; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='42683169']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 42683169, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "d2a442f95e5e5e5a97071e965f30c7b1" } } $('.js-work-strip[data-work-id=42683169]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":42683169,"title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders","translated_title":"","metadata":{"abstract":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.","publication_date":{"day":null,"month":null,"year":2013,"errors":{}}},"translated_abstract":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. The physical properties of the precursor polymer solutions (pH, surface tension, viscosity and conductivity) were measured. The morphological and structural characteristics of the nanoceramic powders were investigated by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The lattice constant, average particle size, microstrain and dislocation density of the samples were calculated. The results show that the average particle size decreased while both the microstrain and the dislocation density values increased in the boron doped indium stabilized bismuth oxide. The structure proposed from FTIR spectra is mainly based on BiO 6 and BiO 3 units.","internal_url":"https://www.academia.edu/42683169/CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders","translated_internal_url":"","created_at":"2020-04-09T16:25:33.957-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":48920836,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":34170036,"work_id":42683169,"tagging_user_id":48920836,"tagged_user_id":48920836,"co_author_invite_id":7008069,"email":"g***e@gmail.com","display_order":1,"name":"özge gökmen","title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders"},{"id":34170037,"work_id":42683169,"tagging_user_id":48920836,"tagged_user_id":820891,"co_author_invite_id":null,"email":"p***u@gmail.com","affiliation":"Gazi University","display_order":2,"name":"Prof.Dr. İbrahim USLU","title":"CERAMICS INTERNATIONAL Structural investigation of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders"}],"downloadable_attachments":[{"id":62892827,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/62892827/thumbnails/1.jpg","file_name":"Ceramics_Intrenational_201320200409-103310-lrnn4v.pdf","download_url":"https://www.academia.edu/attachments/62892827/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"CERAMICS_INTERNATIONAL_Structural_invest.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/62892827/Ceramics_Intrenational_201320200409-103310-lrnn4v-libre.pdf?1586475341=\u0026response-content-disposition=attachment%3B+filename%3DCERAMICS_INTERNATIONAL_Structural_invest.pdf\u0026Expires=1733898196\u0026Signature=JeTtiiugpdmaVaPOikdZzfGyHuS7AxZapGzqwNFH7CLKzgcrzhrRXU0-wGbR1H-HWCdqSfBvOhhxxeLIbnV1LndUAasON4NwyfVcTn7I4~j4Gyygsn5DGXOirYW5BeGuUTvkNruKibjczn-qreg9rUPXB6PFYrakdpkKM77oPyTpqP6rK1R~G9FLoH9hOi9kW7Dr3eGZi47seB-kL3VoGvPR7uH8716Lvv7ZLorRKWIVr9FyDZpF3NsjRQAjX6OYYOAmVGzmYrU9wvQJ1z0ns250EIVO2GVBeh~XV7nJXkvVbSrSNBh6kQOIGC~fEWMvAKjDsmyK5rert1hxA3fojA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"CERAMICS_INTERNATIONAL_Structural_investigation_of_boron_undoped_and_doped_indium_stabilized_bismuth_oxide_nanoceramic_powders","translated_slug":"","page_count":6,"language":"en","content_type":"Work","summary":"The synthesis of boron undoped and doped indium stabilized bismuth oxide nanoceramic powders via the polymeric precursor technique were described. 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The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="341e74b2252352fbf4d5ed18a0176e9b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671641,&quot;asset_id&quot;:36729583,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729583"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729583"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729583; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729583]").text(description); $(".js-view-count[data-work-id=36729583]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729583; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729583']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729583, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "341e74b2252352fbf4d5ed18a0176e9b" } } $('.js-work-strip[data-work-id=36729583]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729583,"title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods","translated_title":"","metadata":{"doi":"10.1007/s12034-018-1602-6","volume":"41","abstract":"Three different thicknesses (50, 150 and 500 nm) Zn-doped polyvinyl alcohol (PVA) was deposited on n-4H-SiC wafer as interlayer by electrospinning method and so, Au/(Zn-doped PVA)/n-4H-SiC metal–polymer–semiconductor structures were fabricated. The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.","page_numbers":"82","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Bulletin of Materials Science"},"translated_abstract":"Three different thicknesses (50, 150 and 500 nm) Zn-doped polyvinyl alcohol (PVA) was deposited on n-4H-SiC wafer as interlayer by electrospinning method and so, Au/(Zn-doped PVA)/n-4H-SiC metal–polymer–semiconductor structures were fabricated. The thickness effect of Zn-doped PVA on the dielectric constant (ε), dielectric loss (ε), loss-tangent (tan δ), real and imaginary parts of electric modulus (M and M) and ac electrical conductivity (σ ac) of them were analysed and compared using experimental capacitance (C) and conductance (G/ω) data in the frequency range of 1–500 kHz at room temperature. According to these results, the values of ε and ε decrease with increasing frequency almost exponentially, σ ac increases especially, at high frequencies. The M and M values were obtained from the ε and ε data and the M and M vs. f plots were drawn for these structures. While the values of ε , ε and tan δ increase with increasing interlayer thickness, the values of M and M decrease with increasing interlayer thickness. The double logarithmic σ ac vs. f plots for each structure have two distinct linear regimes with different slopes, which correspond to low and high frequencies, respectively, and it is prominent that there exist two different conduction mechanisms. Obtained results were found as a strong function of frequency and interlayer thickness.","internal_url":"https://www.academia.edu/36729583/A_comparative_study_on_dielectric_behaviours_of_Au_Zn_doped_PVA_n_4H_SiC_MPS_structures_with_different_interlayer_thicknesses_using_impedance_spectroscopy_methods","translated_internal_url":"","created_at":"2018-05-28T03:06:58.280-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470282,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":6684049,"email":"f***r@sdu.edu.tr","display_order":1,"name":"Ahmet Faruk Özdemir","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470283,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":46531121,"co_author_invite_id":null,"email":"a***l@gazi.edu.tr","display_order":2,"name":"Ş. Altındal","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470284,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":6684050,"email":"v***n@gmail.com","display_order":3,"name":"H. E. Lapa","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"},{"id":31470285,"work_id":36729583,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":4,"name":"A. Kökçe","title":"A comparative study on dielectric behaviours of Au/(Zn-doped PVA)/n-4H-SiC (MPS) structures with different interlayer thicknesses using impedance spectroscopy methods"}],"downloadable_attachments":[{"id":56671641,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671641/thumbnails/1.jpg","file_name":"10.1004.pdf","download_url":"https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_comparative_study_on_dielectric_behavi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671641/10.1004-libre.pdf?1527502376=\u0026response-content-disposition=attachment%3B+filename%3DA_comparative_study_on_dielectric_behavi.pdf\u0026Expires=1733355286\u0026Signature=MjAf1DZdf4pw99sZ1Dze5Esuf15SYtUEDSnlnaHI-8HxzXa8fkSkQAtmlcE1shMywx8vEz3LeQwQs02ByUXNFkZUiphasMaMReMu4M~ColYdNzJqywb1llbBmGDzM54giGzccvGXXQTir3AjAtKeh-O2YGdLvXUvAMmQmLGw3iti3GucRrdMBQnkv0zUYFTrj2xbwJ52hrr4HMPFDG7TLdKTVbbANCFowUBdYgdPfyEtoCdoC6jeUUr2k8Bga-CheNMixUgoJaNSRzUOnuiFOo3eQRhUsfy1IBs2H6T-rgw-ZVrBl9tPAsa~l8U~JAXBagwQBZxrWM1OwKqeiJ9TRQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"A_comparative_study_on_dielectric_behaviours_of_Au_Zn_doped_PVA_n_4H_SiC_MPS_structures_with_different_interlayer_thicknesses_using_impedance_spectroscopy_methods","translated_slug":"","page_count":6,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU","email":"RUVNbEhsVGZqdC94MFVUQnRLQi9oRkNzVndRdUJyNWgxdkd3aWtIRHlGdnhSUVhUQ1RHSmNteDJCT1lsUmYwVi0tNU8wb2kxOHluNm5uelVvcTdKQTVhUT09--02f3c170f13bb37b6d7a70ab31c01b8d2863d08c"},"attachments":[{"id":56671641,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671641/thumbnails/1.jpg","file_name":"10.1004.pdf","download_url":"https://www.academia.edu/attachments/56671641/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_comparative_study_on_dielectric_behavi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671641/10.1004-libre.pdf?1527502376=\u0026response-content-disposition=attachment%3B+filename%3DA_comparative_study_on_dielectric_behavi.pdf\u0026Expires=1733355286\u0026Signature=MjAf1DZdf4pw99sZ1Dze5Esuf15SYtUEDSnlnaHI-8HxzXa8fkSkQAtmlcE1shMywx8vEz3LeQwQs02ByUXNFkZUiphasMaMReMu4M~ColYdNzJqywb1llbBmGDzM54giGzccvGXXQTir3AjAtKeh-O2YGdLvXUvAMmQmLGw3iti3GucRrdMBQnkv0zUYFTrj2xbwJ52hrr4HMPFDG7TLdKTVbbANCFowUBdYgdPfyEtoCdoC6jeUUr2k8Bga-CheNMixUgoJaNSRzUOnuiFOo3eQRhUsfy1IBs2H6T-rgw-ZVrBl9tPAsa~l8U~JAXBagwQBZxrWM1OwKqeiJ9TRQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering"},{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":519,"name":"Solid State Physics","url":"https://www.academia.edu/Documents/in/Solid_State_Physics"},{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":532,"name":"Physical Chemistry","url":"https://www.academia.edu/Documents/in/Physical_Chemistry"},{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles"},{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":23992,"name":"Nanochemistry","url":"https://www.academia.edu/Documents/in/Nanochemistry"},{"id":34550,"name":"Polymer Nanocomposites","url":"https://www.academia.edu/Documents/in/Polymer_Nanocomposites"},{"id":66399,"name":"Synthesis and Characterization of nanomaterials","url":"https://www.academia.edu/Documents/in/Synthesis_and_Characterization_of_nanomaterials"},{"id":91080,"name":"Nano Technology","url":"https://www.academia.edu/Documents/in/Nano_Technology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":1019454,"name":"Nano Fabrication","url":"https://www.academia.edu/Documents/in/Nano_Fabrication"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729558"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures"><img alt="Research paper thumbnail of Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures" class="work-thumbnail" src="https://attachments.academia-assets.com/56671613/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures">Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures</a></div><div class="wp-workCard_item"><span>Journal of Electronic Materials</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) s...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63436e5bb95fa4027fc62470378091d9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671613,&quot;asset_id&quot;:36729558,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671613/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729558"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729558"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729558; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729558]").text(description); $(".js-view-count[data-work-id=36729558]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729558; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729558']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729558, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "63436e5bb95fa4027fc62470378091d9" } } $('.js-work-strip[data-work-id=36729558]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729558,"title":"Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures","translated_title":"","metadata":{"doi":"10.1007/s11664-018-6195-8","abstract":"The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Journal of Electronic Materials"},"translated_abstract":"The aim of this study is to improve the electrical property of Ag/n-Si metal–semiconductor (MS) structure by growing an Ru-doped PVP interlayer between Ag and n-Si using electrospinning technique. To illustrate the utility of the Ru-doped PVP interface layer, current–voltage (I–V) characteristics of Ag/n-Si (MS) and Ag/Ru-doped PVP/n-Si metal–polymer–semiconductor (MPS) structures was carried out. In addition, the main electrical parameters of the fabricated Ag/Ru-doped PVP/n-Si structures were investigated as a function of frequency and electric field using impedance spectroscopy method (ISM). The capacitance–voltage (C–V) plot showed an anomalous peak in the depletion region due to the special density distribution of interface traps/states (Dit/Nss) and interlayer. Both the values of series resistance (Rs) and Nss were drawn as a function of voltage and frequency between 0.5 kHz and 5 MHz at room temperature and they had a peak behavior in the depletion region. Some important parameters of the sample such as the donor concentration atoms (ND), Fermi energy (E F ), thickness of the depletion region (WD), barrier height (Φ B0 ) and R s were determined from the C−2 versus V plot for each frequency. The values of N D , W D , Φ B0 and R s were changed from 1 × 1015 cm−3, 9.61 × 10−5 cm, 0.94 eV and 19,055 Ω (at 0.5 kHz) to 0.13 × 1015 cm−3, 27.4 × 10−4 cm, 1.04 eV and 70 Ω (at 5 MHz), respectively. As a result of the experiments, it is observed that the change in electrical parameters becomes more effective at lower frequencies due to the Nss and their relaxation time (τ), dipole and surface polarizations.","internal_url":"https://www.academia.edu/36729558/Effects_of_a_Thin_Ru_Doped_PVP_Interface_Layer_on_Electrical_Behavior_of_Ag_n_Si_Structures","translated_internal_url":"","created_at":"2018-05-28T03:00:43.625-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470255,"work_id":36729558,"tagging_user_id":820891,"tagged_user_id":1303640,"co_author_invite_id":null,"email":"b***f@gmail.com","affiliation":"İstanbul Ticaret Üniversitesi","display_order":1,"name":"Yosef badali","title":"Effects of a Thin Ru-Doped PVP Interface Layer on Electrical Behavior of Ag/n-Si Structures"},{"id":31470256,"work_id":36729558,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":3,"name":"A. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729519"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure"><img alt="Research paper thumbnail of On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure" class="work-thumbnail" src="https://attachments.academia-assets.com/56671568/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure">On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure</a></div><div class="wp-workCard_item"><span>Journal of Materials Science: Materials in Electronics</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="fef1eda6f8eed5bba58e59f896acd832" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671568,&quot;asset_id&quot;:36729519,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671568/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729519; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729519]").text(description); $(".js-view-count[data-work-id=36729519]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729519; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729519']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729519, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "fef1eda6f8eed5bba58e59f896acd832" } } $('.js-work-strip[data-work-id=36729519]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729519,"title":"On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure","translated_title":"","metadata":{"doi":"10.1007/s10854-017-8219-1","volume":"29","abstract":"The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","page_numbers":"2890-2898","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Journal of Materials Science: Materials in Electronics"},"translated_abstract":"The frequency and voltage dependence of the capacitance–voltage (C–V) and conductance–voltage (G/ω–V) characteristics of the Al/(%7 Zn-doped PVA)/p-Si (MPS) structure were investigated in the wide range of frequency and voltage. Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","internal_url":"https://www.academia.edu/36729519/On_the_anomalous_peak_and_negative_capacitance_in_the_capacitance_voltage_C_V_plots_of_Al_7_Zn_PVA_p_Si_MPS_structure","translated_internal_url":"","created_at":"2018-05-28T02:52:30.827-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":31470237,"work_id":36729519,"tagging_user_id":820891,"tagged_user_id":46531121,"co_author_invite_id":null,"email":"a***l@gazi.edu.tr","display_order":1,"name":"Ş. Altındal","title":"On the anomalous peak and negative capacitance in the capacitance–voltage (C–V) plots of Al/(%7 Zn-PVA)/p-Si (MPS) structure"},{"id":31470238,"work_id":36729519,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":1009690,"email":"u***5@yahoo.com","display_order":3,"name":"E. E. 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Frequency and voltage dependence of C and G/ω shows that these parameters are functions of frequency and voltage. The C–V plot has an anomalous peak and an intersection/crossing point around 1.4 V after which C becomes negative. This negative capaci-tance (NC) phenomena was attributed to the surface states (N ss), series resistance (R s) and minority carrier injection. The intensity of NC decreases with increasing frequency and the minimum value of C corresponds to the maximum value of G/ω at strong accumulation region. Whereas the C–V plots have only one peak at low frequencies, they have two peaks at high frequencies due to the special density distribution of N ss and their relaxation time. In addition, the changes in the C and G/ω were attributed to the increase in the polarization and the increased number of carriers in the structure. Impedance method was used for calculation of R s whereas N ss was obtained using two methods; (i) the high–low frequency capacitance and (ii) Hill-Coleman method as a function of voltage and frequency, respectively. The Fermi energy level (E F), the concentration of doping acceptor atoms (N A) and barrier height (Φ B) values were obtained from reverse bias C −2 vs V plots for each frequency.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":56671568,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/56671568/thumbnails/1.jpg","file_name":"on_the_ana.pdf","download_url":"https://www.academia.edu/attachments/56671568/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"On_the_anomalous_peak_and_negative_capac.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/56671568/on_the_ana-libre.pdf?1527501526=\u0026response-content-disposition=attachment%3B+filename%3DOn_the_anomalous_peak_and_negative_capac.pdf\u0026Expires=1733756524\u0026Signature=drVeJNG3fDWtBqg3DGDExLK6OixBhfnMMVMslIE54tnfjfct7kiafbYhJB1-TALyG7XMPDjnYfIUE-DAOUjBcA6mO~cmsKKBVZulxM0I3NKeQEslPSJyztE7Lw9d9gNEsGh-53cyHwcn6pMlYCQYNdXhOkvTlt1q37fMg1bQj-~I2JALya9~hcBY0cqNGkICVcLYgksP-j~DY~g2SZv35aL3jlw86pvz3jIlfJFFqXEsNnJeKp6Y3SWvhP-F0VqsWK9y2DvxT76vlrZZEOVcTHatrlHzBQQUhitIG1-g0ioRu9IBqgxRzDsvzzp4a22y95lvoCcDC48~rf6J1W4Axw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":3848,"name":"Nanomaterials Characterization","url":"https://www.academia.edu/Documents/in/Nanomaterials_Characterization"},{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics"},{"id":11678,"name":"Nanocomposites","url":"https://www.academia.edu/Documents/in/Nanocomposites"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials"},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience"},{"id":144046,"name":"Frequency","url":"https://www.academia.edu/Documents/in/Frequency"},{"id":389165,"name":"Voltage","url":"https://www.academia.edu/Documents/in/Voltage"}],"urls":[{"id":8509618,"url":"https://link.springer.com/article/10.1007%2Fs10854-017-8219-1"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="36729474"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/36729474/Thermoelectric_Properties_of_nickel_and_boron_co_substituted_Prepared_by_Electrospinning_Technique"><img alt="Research paper thumbnail of Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique" class="work-thumbnail" src="https://attachments.academia-assets.com/56671526/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/36729474/Thermoelectric_Properties_of_nickel_and_boron_co_substituted_Prepared_by_Electrospinning_Technique">Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique</a></div><div class="wp-workCard_item"><span> Nano Hybrids and Composites</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic p...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic powders were synthesized using electrospinning techniques and then consolidated into bulk ceramics. The differences in the microstructure and thermoelectric properties of the samples as a result of doping effect have been investigated. The crystalline structures of the powders and nanofibers were characterized using X-ray diffraction and scanning electron microscopy and BET Analysis before and after the calcination process at different temperatures. Nanofibers prepared by the use of electrospinning technique, have a diameter of approximately 300 nm, and the diameter of the grains of calcined powders was observed to range between 150 to 500 nanometers. Thermoelectric properties of the bulk ceramics were measured by physical properties measurement system (Lot-Oriel PPMS) in a temperature range of 15–300 K. The calculated values of dimensionless figure of merit at 300 K are , , and for sintered powders from undoped, Ni and B doped powders, respectively.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="117c5104cbaee706f452fcfeaf238939" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:56671526,&quot;asset_id&quot;:36729474,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/56671526/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="36729474"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="36729474"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36729474; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36729474]").text(description); $(".js-view-count[data-work-id=36729474]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36729474; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='36729474']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 36729474, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "117c5104cbaee706f452fcfeaf238939" } } $('.js-work-strip[data-work-id=36729474]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":36729474,"title":"Thermoelectric Properties of nickel and boron co-substituted Prepared by Electrospinning Technique","translated_title":"","metadata":{"doi":"10.4028/www.scientific.net/NHC.19.34","volume":"19","abstract":"In this study nickel and boron doped sodium cobalt oxide-nanocrystalline thermoelectric ceramic powders were synthesized using electrospinning techniques and then consolidated into bulk ceramics. 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Bu amaçla 5 farklı polimer çözelti hazırlanmış olup bu çözeltilerden 4 tanesi elektro-eğirme yöntemi ile nanolif haline dönüştürülmüştür. Diğer örnek ise polimerik sol-jel metodu ile üretilmiştir. Her iki yöntemle üretilen numuneler kalsinasyon işlemine tabi tutularak toz halinde termoelektrik nanokompozit seramik malzemeler elde edilmiştir. Nanoliflerin kalsinasyon işlemi öncesi ve sonrasındaki morfolojileri taramalı elektron mikroskobu ile incelenmiştir. Numunelerin yapısal analizi XRD cihazı ve kızıl ötesi spektrometresi (FTIR) ile karakterize edilmiştir. Aynı zamanda elektro-eğirme yöntemi ile üretilen numunelerin termal özellikleri, DSC, TGA ve DTA ölçümleri ile belirlenmiştir. Daha sonra, toz halindeki malzemeler soğuk pres yöntemiyle pelet haline getirilmiş ve uygun sıcaklıkta sinterleme işlemine tabi tutulmuştur. Sinterleme sonrası bütün numunelerin termoelektrik özellikleri (Seebeck katsayısı, elektriksel iletkenlik, ısıl iletkenlik, termoelektrik değer katsayısı) 10-300 K sıcaklıkları arasında Lot – Oriel PPMS ölçüm sistemi ile ölçülmüştür. 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Bu amaçla 5 farklı polimer çözelti hazırlanmış olup bu çözeltilerden 4 tanesi elektro-eğirme yöntemi ile nanolif haline dönüştürülmüştür. Diğer örnek ise polimerik sol-jel metodu ile üretilmiştir. Her iki yöntemle üretilen numuneler kalsinasyon işlemine tabi tutularak toz halinde termoelektrik nanokompozit seramik malzemeler elde edilmiştir. Nanoliflerin kalsinasyon işlemi öncesi ve sonrasındaki morfolojileri taramalı elektron mikroskobu ile incelenmiştir. Numunelerin yapısal analizi XRD cihazı ve kızıl ötesi spektrometresi (FTIR) ile karakterize edilmiştir. Aynı zamanda elektro-eğirme yöntemi ile üretilen numunelerin termal özellikleri, DSC, TGA ve DTA ölçümleri ile belirlenmiştir. Daha sonra, toz halindeki malzemeler soğuk pres yöntemiyle pelet haline getirilmiş ve uygun sıcaklıkta sinterleme işlemine tabi tutulmuştur. Sinterleme sonrası bütün numunelerin termoelektrik özellikleri (Seebeck katsayısı, elektriksel iletkenlik, ısıl iletkenlik, termoelektrik değer katsayısı) 10-300 K sıcaklıkları arasında Lot – Oriel PPMS ölçüm sistemi ile ölçülmüştür. Sonuç olarak, üretim yönteminin ve sodyum kobaltit içerisine eklenen Ni, B katkılarının termoelektrik özellikler üzerindeki etkileri ayrıntılı olarak incelenmiştir.\r\n"},"translated_abstract":"\r\nBu kitapta oksit termoelektrik madde olarak bilinen sodyum kobaltit ( NaxCo2O4 ) ve onun nikel ve bor katkılı türevleri elektro-eğirme metoduyla üretilerek fiziksel ve termoelektrik özellikleri incelenmiştir. Bu amaçla 5 farklı polimer çözelti hazırlanmış olup bu çözeltilerden 4 tanesi elektro-eğirme yöntemi ile nanolif haline dönüştürülmüştür. Diğer örnek ise polimerik sol-jel metodu ile üretilmiştir. Her iki yöntemle üretilen numuneler kalsinasyon işlemine tabi tutularak toz halinde termoelektrik nanokompozit seramik malzemeler elde edilmiştir. Nanoliflerin kalsinasyon işlemi öncesi ve sonrasındaki morfolojileri taramalı elektron mikroskobu ile incelenmiştir. Numunelerin yapısal analizi XRD cihazı ve kızıl ötesi spektrometresi (FTIR) ile karakterize edilmiştir. Aynı zamanda elektro-eğirme yöntemi ile üretilen numunelerin termal özellikleri, DSC, TGA ve DTA ölçümleri ile belirlenmiştir. Daha sonra, toz halindeki malzemeler soğuk pres yöntemiyle pelet haline getirilmiş ve uygun sıcaklıkta sinterleme işlemine tabi tutulmuştur. Sinterleme sonrası bütün numunelerin termoelektrik özellikleri (Seebeck katsayısı, elektriksel iletkenlik, ısıl iletkenlik, termoelektrik değer katsayısı) 10-300 K sıcaklıkları arasında Lot – Oriel PPMS ölçüm sistemi ile ölçülmüştür. Sonuç olarak, üretim yönteminin ve sodyum kobaltit içerisine eklenen Ni, B katkılarının termoelektrik özellikler üzerindeki etkileri ayrıntılı olarak incelenmiştir.\r\n","internal_url":"https://www.academia.edu/11407268/Elektrospin_Y%C3%B6ntemiyle_Thermoelektrik_Nano_Yap%C4%B1lar_%C3%9Cretimi","translated_internal_url":"","created_at":"2015-03-13T06:48:39.840-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"book","co_author_tags":[{"id":264195,"work_id":11407268,"tagging_user_id":820891,"tagged_user_id":null,"co_author_invite_id":109475,"email":"m***u@selcuk.edu.tr","display_order":null,"name":"Mustafa Koyuncu","title":"Elektrospin Yöntemiyle Thermoelektrik Nano Yapılar Üretimi"}],"downloadable_attachments":[{"id":36961841,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/36961841/thumbnails/1.jpg","file_name":"978-3-639-67254-1.pdf","download_url":"https://www.academia.edu/attachments/36961841/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Elektrospin_Yontemiyle_Thermoelektrik_Na.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/36961841/978-3-639-67254-1-libre.pdf?1426253098=\u0026response-content-disposition=attachment%3B+filename%3DElektrospin_Yontemiyle_Thermoelektrik_Na.pdf\u0026Expires=1733756524\u0026Signature=NcrhK2KZd-2Awa-E03PwSuGmloU0CMsccmgJ4e2OQxhoEXCiUyaK~BWWKzeRYxVldW~lxbqlvLfAv~nwTjvTY4iNGUjaFZHm0zkjkWQMVxbqRGTUWTIkpbgPCWRhoGuAkU0-iBIupv25hljE9l6uacyX3018cyyOftxCaixSraGhki61AxWncNRXHyArJWDjauePdaZHSUmWUHUkkQaDl72Y95puHkYp6QwTHtxTFjI~cWvyPZNsQ~AjZyg6dIhMrmE~LJHn1O5Lxh2yi46twy6aX1RCwBW5406hewfj4Ww36dn1w4VQBKH7Z7z5kAWVseswe1oZ~d3dA13k42TIZA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Elektrospin_Yöntemiyle_Thermoelektrik_Nano_Yapılar_Üretimi","translated_slug":"","page_count":97,"language":"tr","content_type":"Work","summary":"\r\nBu kitapta oksit termoelektrik madde olarak bilinen sodyum kobaltit ( NaxCo2O4 ) ve onun nikel ve bor katkılı türevleri elektro-eğirme metoduyla üretilerek fiziksel ve termoelektrik özellikleri incelenmiştir. Bu amaçla 5 farklı polimer çözelti hazırlanmış olup bu çözeltilerden 4 tanesi elektro-eğirme yöntemi ile nanolif haline dönüştürülmüştür. Diğer örnek ise polimerik sol-jel metodu ile üretilmiştir. Her iki yöntemle üretilen numuneler kalsinasyon işlemine tabi tutularak toz halinde termoelektrik nanokompozit seramik malzemeler elde edilmiştir. Nanoliflerin kalsinasyon işlemi öncesi ve sonrasındaki morfolojileri taramalı elektron mikroskobu ile incelenmiştir. Numunelerin yapısal analizi XRD cihazı ve kızıl ötesi spektrometresi (FTIR) ile karakterize edilmiştir. Aynı zamanda elektro-eğirme yöntemi ile üretilen numunelerin termal özellikleri, DSC, TGA ve DTA ölçümleri ile belirlenmiştir. Daha sonra, toz halindeki malzemeler soğuk pres yöntemiyle pelet haline getirilmiş ve uygun sıcaklıkta sinterleme işlemine tabi tutulmuştur. Sinterleme sonrası bütün numunelerin termoelektrik özellikleri (Seebeck katsayısı, elektriksel iletkenlik, ısıl iletkenlik, termoelektrik değer katsayısı) 10-300 K sıcaklıkları arasında Lot – Oriel PPMS ölçüm sistemi ile ölçülmüştür. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1444058"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1444058/Elektrospinleme_Y%C3%B6ntemi_ile_Seramik_Nano_Borkarb%C3%BCr_%C3%9Cretimi_ve_Karekterizasyonu_Elektrospinleme_Y%C3%B6ntemi_ile_Seramik_Nano_Borkarb%C3%BCr_%C3%9Cretimi_ve_Karekterizasyonu"><img alt="Research paper thumbnail of Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu" class="work-thumbnail" src="https://attachments.academia-assets.com/11524663/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1444058/Elektrospinleme_Y%C3%B6ntemi_ile_Seramik_Nano_Borkarb%C3%BCr_%C3%9Cretimi_ve_Karekterizasyonu_Elektrospinleme_Y%C3%B6ntemi_ile_Seramik_Nano_Borkarb%C3%BCr_%C3%9Cretimi_ve_Karekterizasyonu">Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">English Boron is one of the most strategically important materials for the development of our co...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">English<br /><br />Boron is one of the most strategically important materials for the development of our country. Turkey has almost 74 % of the total world boron reserves. Boron, used in many fields of industry, is exported outside without any added value. Therefore the cooperation between the industry and universities is of paramount importance for the proper use of this strategically important element. We are hoping that the four patents prepared as a result of this project will be of benefit for the industry <br />The book involves the production of nano fibers PVA/BA solutions by the use of electrospinning technique. There have been more than fifteen papers published related to the nano fibers produced by the addition of various metals and compound the different polymer and copolymer solutions. Among these are nano technical studies related to conductive polymers, Shottky diodes, wound dressing materials , nano-wires and thermo electrical materials. It is thought that the study has reached far beyond its original objectives .<br />There are various institutions who opened their facilities for our use. We would like to express our sincere gratitude to Prof.Dr. Güngör GÜNDÜZ, who is also the consultant of the project , for letting us use his laboratories in Middle East universities. Thanks are also due to MAT office of Turkish Mineral research and Exploration Institute for allowing us to use their laboratories, Dr. Evren ÇUBUKÇU and Orkun ERSOY for SEM analyses, Prof.Dr. Kadir PEKMEZ and Dr. Fulya CANLI for the use of four point probe conductivity device and Prof.Dr. Mehmet Mutlu and Dr. Nesrin KIR for the use of the research facilities in their labs. <br /><br />Turkish<br /><br />Bor ülkemizin kalkınmasında en önemli stratejik maddelerden biridir. Dünya bor rezervlerinin yaklaşık %74’ü ülkemizde bulunmaktadır. Pek çok sanayi ve teknoloji dalında yaygın biçimde kullanılan bor yurt dışına hiç bir katma değer katılmadan satmaktadır. Gelecekte stratejik önemi olan bor konusunda üniversite-sanayi işbirliği önemlidir. Bu kitabın hazırlanmasında 106T630 nolu TUBİTAK projesinin katkıları olmuştur. Bu projeyi çok değerli meslaktaşlarım Prof.Dr. Mehmet Levent AKSU ve Yard.Doç.Dr. Hüseyin ÇELİKKAN ile yüksek lisans öğrencim Hatice DAŞTAN’ın önemli katkıları ile tamamladım. Özellikle çalışmalarımın önemli bir bölümü Sn. AKSU’nun labaratuarlarında gerçekleşmiştir. Teşekkürü borç bilirim. Bu iki meslaktaşımla daha pek çok bilimsel çalışmada birlikte olmaktan mutluluk duyacağım. Projenin sayesinde hazırlanan dört patent başvurusu TUBİTAK tarafından da teşvik almış ve yurt dışı incelemesi için gerekli başvurular yapılmıştır. Bu patentlerin ülkemiz sanayinde kullanılmasını görmek bizleri çok mutlu edecektir. Ayrıca bu proje sayesinde hazırlanan nanokompozit malzemelerden üretilen süper iletken malzemeler, iletken polimerler, schotky diyotlar, yara sargı materyalleri, nanoteller, termo elektrik materyaller gibi değişik alanlarda nanoteknolojik çalışmalar yapılmıştır. Bu çalışmalarda Doç.Dr. Şemsettin ALTINDAL, Doç.Dr. İlbilge DÖKME, Yard.Doç.Dr. Tuncay TUNÇ gibi değerli akademisyenlerde yer almışlardır. Çalışmaların çoğu yurt dışı dergilerde yayınlanmıştır. Devletimizin kıt kaynaklarından ayırarak bize verdiği proje bedelini üstün bir şekilde çalışarak, hazırladığımız patentlerle ve yayınlarla ülkemizin bilimsel gelişmesine katkıda bulunarak geri vermeye çalıştık. Bu projede bazı üniversiteler bize laboratuar olanaklarını açarak katkıda bulunmuşlardır. En başta ayni zamanda proje danışmanımız Prof.Dr. Güngör GÜNDÜZ bize ODTÜ Kimya Mühendisliği Bölümündeki Nükleer Uygulama Laboratuarını açarak imkânlarından bizi yararlandırmıştır. Bir süreliğine de olsa Maden tetkik ve Araştırma Genel Müdürlüğü’de MAT Dairesi Başkanlığına ait laboratuar imkanlarından bizi yararlandırmıştır. Aynı zamanda Hacettepe Üniversitesinde; Jeoloji Mühendisliği Bölümünde bulunan SEM imkanlarından bizleri yararlandıran Dr. Evren ÇUBUKÇU’ya ve Orkun ERSOY’a, Kimya Bölümünde bulunan dört nokta prob cihazını kullandıran kullandıran Prof.Dr. kadir PEKMEZ ve Dr. Fulya CANLI’ya, Gıda mühendisliği Bölümündeki laboratuarı imkanlarından bizi yararlandıran Prof.Dr. Mehmet Mutlu’ya ve Dr. Nesrin ŞİR’e yardımlarından dolayı teşekkürlerimizi sunarız. <br /><br /><br />Key words : Electro –spinning , PVA, Boron carbide , boric acid , nanotechnology , micro wave sintering</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b6906b11b0eac5404b49160c3b659b19" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:11524663,&quot;asset_id&quot;:1444058,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/11524663/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1444058"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1444058"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1444058; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1444058]").text(description); $(".js-view-count[data-work-id=1444058]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1444058; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1444058']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1444058, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b6906b11b0eac5404b49160c3b659b19" } } $('.js-work-strip[data-work-id=1444058]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1444058,"title":"Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu Elektrospinleme Yöntemi ile Seramik Nano Borkarbür Üretimi ve Karekterizasyonu","translated_title":"","metadata":{"abstract":"English\n\nBoron is one of the most strategically important materials for the development of our country. Turkey has almost 74 % of the total world boron reserves. Boron, used in many fields of industry, is exported outside without any added value. Therefore the cooperation between the industry and universities is of paramount importance for the proper use of this strategically important element. We are hoping that the four patents prepared as a result of this project will be of benefit for the industry \nThe book involves the production of nano fibers PVA/BA solutions by the use of electrospinning technique. There have been more than fifteen papers published related to the nano fibers produced by the addition of various metals and compound the different polymer and copolymer solutions. Among these are nano technical studies related to conductive polymers, Shottky diodes, wound dressing materials , nano-wires and thermo electrical materials. It is thought that the study has reached far beyond its original objectives .\nThere are various institutions who opened their facilities for our use. We would like to express our sincere gratitude to Prof.Dr. Güngör GÜNDÜZ, who is also the consultant of the project , for letting us use his laboratories in Middle East universities. Thanks are also due to MAT office of Turkish Mineral research and Exploration Institute for allowing us to use their laboratories, Dr. Evren ÇUBUKÇU and Orkun ERSOY for SEM analyses, Prof.Dr. Kadir PEKMEZ and Dr. Fulya CANLI for the use of four point probe conductivity device and Prof.Dr. Mehmet Mutlu and Dr. Nesrin KIR for the use of the research facilities in their labs. \n\nTurkish\n\nBor ülkemizin kalkınmasında en önemli stratejik maddelerden biridir. Dünya bor rezervlerinin yaklaşık %74’ü ülkemizde bulunmaktadır. Pek çok sanayi ve teknoloji dalında yaygın biçimde kullanılan bor yurt dışına hiç bir katma değer katılmadan satmaktadır. Gelecekte stratejik önemi olan bor konusunda üniversite-sanayi işbirliği önemlidir. Bu kitabın hazırlanmasında 106T630 nolu TUBİTAK projesinin katkıları olmuştur. Bu projeyi çok değerli meslaktaşlarım Prof.Dr. Mehmet Levent AKSU ve Yard.Doç.Dr. Hüseyin ÇELİKKAN ile yüksek lisans öğrencim Hatice DAŞTAN’ın önemli katkıları ile tamamladım. Özellikle çalışmalarımın önemli bir bölümü Sn. AKSU’nun labaratuarlarında gerçekleşmiştir. Teşekkürü borç bilirim. Bu iki meslaktaşımla daha pek çok bilimsel çalışmada birlikte olmaktan mutluluk duyacağım. Projenin sayesinde hazırlanan dört patent başvurusu TUBİTAK tarafından da teşvik almış ve yurt dışı incelemesi için gerekli başvurular yapılmıştır. Bu patentlerin ülkemiz sanayinde kullanılmasını görmek bizleri çok mutlu edecektir. Ayrıca bu proje sayesinde hazırlanan nanokompozit malzemelerden üretilen süper iletken malzemeler, iletken polimerler, schotky diyotlar, yara sargı materyalleri, nanoteller, termo elektrik materyaller gibi değişik alanlarda nanoteknolojik çalışmalar yapılmıştır. Bu çalışmalarda Doç.Dr. Şemsettin ALTINDAL, Doç.Dr. İlbilge DÖKME, Yard.Doç.Dr. Tuncay TUNÇ gibi değerli akademisyenlerde yer almışlardır. Çalışmaların çoğu yurt dışı dergilerde yayınlanmıştır. Devletimizin kıt kaynaklarından ayırarak bize verdiği proje bedelini üstün bir şekilde çalışarak, hazırladığımız patentlerle ve yayınlarla ülkemizin bilimsel gelişmesine katkıda bulunarak geri vermeye çalıştık. Bu projede bazı üniversiteler bize laboratuar olanaklarını açarak katkıda bulunmuşlardır. En başta ayni zamanda proje danışmanımız Prof.Dr. Güngör GÜNDÜZ bize ODTÜ Kimya Mühendisliği Bölümündeki Nükleer Uygulama Laboratuarını açarak imkânlarından bizi yararlandırmıştır. Bir süreliğine de olsa Maden tetkik ve Araştırma Genel Müdürlüğü’de MAT Dairesi Başkanlığına ait laboratuar imkanlarından bizi yararlandırmıştır. Aynı zamanda Hacettepe Üniversitesinde; Jeoloji Mühendisliği Bölümünde bulunan SEM imkanlarından bizleri yararlandıran Dr. Evren ÇUBUKÇU’ya ve Orkun ERSOY’a, Kimya Bölümünde bulunan dört nokta prob cihazını kullandıran kullandıran Prof.Dr. kadir PEKMEZ ve Dr. Fulya CANLI’ya, Gıda mühendisliği Bölümündeki laboratuarı imkanlarından bizi yararlandıran Prof.Dr. Mehmet Mutlu’ya ve Dr. Nesrin ŞİR’e yardımlarından dolayı teşekkürlerimizi sunarız. \n\n\nKey words : Electro –spinning , PVA, Boron carbide , boric acid , nanotechnology , micro wave sintering","more_info":"İbrahim USLU"},"translated_abstract":"English\n\nBoron is one of the most strategically important materials for the development of our country. Turkey has almost 74 % of the total world boron reserves. Boron, used in many fields of industry, is exported outside without any added value. Therefore the cooperation between the industry and universities is of paramount importance for the proper use of this strategically important element. We are hoping that the four patents prepared as a result of this project will be of benefit for the industry \nThe book involves the production of nano fibers PVA/BA solutions by the use of electrospinning technique. There have been more than fifteen papers published related to the nano fibers produced by the addition of various metals and compound the different polymer and copolymer solutions. Among these are nano technical studies related to conductive polymers, Shottky diodes, wound dressing materials , nano-wires and thermo electrical materials. It is thought that the study has reached far beyond its original objectives .\nThere are various institutions who opened their facilities for our use. We would like to express our sincere gratitude to Prof.Dr. Güngör GÜNDÜZ, who is also the consultant of the project , for letting us use his laboratories in Middle East universities. Thanks are also due to MAT office of Turkish Mineral research and Exploration Institute for allowing us to use their laboratories, Dr. Evren ÇUBUKÇU and Orkun ERSOY for SEM analyses, Prof.Dr. Kadir PEKMEZ and Dr. Fulya CANLI for the use of four point probe conductivity device and Prof.Dr. Mehmet Mutlu and Dr. Nesrin KIR for the use of the research facilities in their labs. \n\nTurkish\n\nBor ülkemizin kalkınmasında en önemli stratejik maddelerden biridir. Dünya bor rezervlerinin yaklaşık %74’ü ülkemizde bulunmaktadır. Pek çok sanayi ve teknoloji dalında yaygın biçimde kullanılan bor yurt dışına hiç bir katma değer katılmadan satmaktadır. Gelecekte stratejik önemi olan bor konusunda üniversite-sanayi işbirliği önemlidir. Bu kitabın hazırlanmasında 106T630 nolu TUBİTAK projesinin katkıları olmuştur. Bu projeyi çok değerli meslaktaşlarım Prof.Dr. Mehmet Levent AKSU ve Yard.Doç.Dr. Hüseyin ÇELİKKAN ile yüksek lisans öğrencim Hatice DAŞTAN’ın önemli katkıları ile tamamladım. Özellikle çalışmalarımın önemli bir bölümü Sn. AKSU’nun labaratuarlarında gerçekleşmiştir. Teşekkürü borç bilirim. Bu iki meslaktaşımla daha pek çok bilimsel çalışmada birlikte olmaktan mutluluk duyacağım. Projenin sayesinde hazırlanan dört patent başvurusu TUBİTAK tarafından da teşvik almış ve yurt dışı incelemesi için gerekli başvurular yapılmıştır. Bu patentlerin ülkemiz sanayinde kullanılmasını görmek bizleri çok mutlu edecektir. Ayrıca bu proje sayesinde hazırlanan nanokompozit malzemelerden üretilen süper iletken malzemeler, iletken polimerler, schotky diyotlar, yara sargı materyalleri, nanoteller, termo elektrik materyaller gibi değişik alanlarda nanoteknolojik çalışmalar yapılmıştır. Bu çalışmalarda Doç.Dr. Şemsettin ALTINDAL, Doç.Dr. İlbilge DÖKME, Yard.Doç.Dr. Tuncay TUNÇ gibi değerli akademisyenlerde yer almışlardır. Çalışmaların çoğu yurt dışı dergilerde yayınlanmıştır. Devletimizin kıt kaynaklarından ayırarak bize verdiği proje bedelini üstün bir şekilde çalışarak, hazırladığımız patentlerle ve yayınlarla ülkemizin bilimsel gelişmesine katkıda bulunarak geri vermeye çalıştık. Bu projede bazı üniversiteler bize laboratuar olanaklarını açarak katkıda bulunmuşlardır. En başta ayni zamanda proje danışmanımız Prof.Dr. Güngör GÜNDÜZ bize ODTÜ Kimya Mühendisliği Bölümündeki Nükleer Uygulama Laboratuarını açarak imkânlarından bizi yararlandırmıştır. Bir süreliğine de olsa Maden tetkik ve Araştırma Genel Müdürlüğü’de MAT Dairesi Başkanlığına ait laboratuar imkanlarından bizi yararlandırmıştır. Aynı zamanda Hacettepe Üniversitesinde; Jeoloji Mühendisliği Bölümünde bulunan SEM imkanlarından bizleri yararlandıran Dr. Evren ÇUBUKÇU’ya ve Orkun ERSOY’a, Kimya Bölümünde bulunan dört nokta prob cihazını kullandıran kullandıran Prof.Dr. kadir PEKMEZ ve Dr. Fulya CANLI’ya, Gıda mühendisliği Bölümündeki laboratuarı imkanlarından bizi yararlandıran Prof.Dr. Mehmet Mutlu’ya ve Dr. Nesrin ŞİR’e yardımlarından dolayı teşekkürlerimizi sunarız. \n\n\nKey words : Electro –spinning , PVA, Boron carbide , boric acid , nanotechnology , micro wave 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src="https://attachments.academia-assets.com/11200285/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1449165/Transient_Response_of_a_Distillation_Column">Transient Response of a Distillation Column</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The object of this,work is to, determine how the mathematical model would predict the dynamic res...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The object of this,work is to, determine how the mathematical model would predict the dynamic response of a pilot plant scale distillation column under extreme transient conditions, and to demonstrate the usefulness of the model in feed-forward control of &#39;the column. The data from the column will be compared with the calculated results. The comparison serves as a test for the mathematical model and its computer program. The control of distillation columns has received a considerably large interest in recent years. Because the separation processes by distillation are found an almost every phase of the chemical and petroleum industries. In order to ensure smooth and economic operation of the distillation column, flows of cooling, heating media and intermediate product should be disturbed as little as possible. Thus, an accurate control of product compositions and column performance is very important. A computer program· is developed for dynamic simulation of the column. The nonlinear equations of the dynamic model are solved numerically. This model requires simultaneous solution of over-all material balances, heat balances, equilibrium and efficiency relationships for each plate. condenser and the reboiler of the column. The component mole balance establishes the liquid flowrate. The vapor liquid relationships establish the vapor composition where<br />as the overall heat balance defines the vapor flow leaving the plate. The binary system of methanol-tertiary butyl alcohol is distilled in,twentyplate, which 10 cm internal diameter bubble cap distillation column which is made of glass.<br /><br />Turkish<br /><br />Bu calışmanın amacı pilot· tesis düzeyinde gecici durum şartlarındaçalışan bir damıtma kulesinin· dinamik tepkilerinin matematiksel model ile tahminini hesaplamaktır. Bir ikinci amacı da bu modelin ileri-beslemeli kule kontrolündak faydasını saptamaktır. Bu amaç için bir damitma kulesinde elde edilen veriler matematiksel model icin yazılan bilgisayar programı sonuclarıyla karılaştırılmıştır. Damıtma kulelerinin koritrolu son yıllarda büyük önem kazanmıştır. Çünkü damıtma ile ayırma işlemleri bütün kimya ve petrol sanayiinde geniş bir şekilde kullanılmaktadır. Damıtma kulelerinin düzenli ve ekonomik calışmaları için soğutma ve ısıtma ayrıca ara ürünlerinin sıcaklığı ve derişimlerinin öngörülen belli sınırlar içinde kalması gerekir. Bu nedenle damıtma kulelerinin iyi bir şekilde kontrol edilmesi önemlidir. Damıtma kulesinin çalışması hakkındaki dinamik model icin bir bilgisayar programı yazılmıştır. Bu·programdaki doğrusal olmayan denklemler nümerik metodla çözülmüştür. Bu cözümde her bir tepsi ve yoğuşturucu ile kazan için genel madde denkliği, ısı denkliği ve verim bağıntıları yer almaktadır. Sıvı akım hızları her bir bileşen için yazılan molar denkliklerle bulunmuştur. Buhar deişimleri buhar-sıvı denge bağıntısıyla, bir tepsiyi terkesen buharın hızıda genel ısı denkliğiyle bulunmuştur. Bu çalışmada deneysel veriler methanol-tersiyer bütül alkol karışımı ile, 10 cm çapındaki yirmi tepsili camdan yapılmış bir damıtma kulesinde elde edilmiştir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="328ddb8da421fa8663df4b32d66abab9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:11200285,&quot;asset_id&quot;:1449165,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/11200285/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1449165"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1449165"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1449165; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1449165]").text(description); $(".js-view-count[data-work-id=1449165]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1449165; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1449165']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1449165, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "328ddb8da421fa8663df4b32d66abab9" } } $('.js-work-strip[data-work-id=1449165]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1449165,"title":"Transient Response of a Distillation Column","translated_title":"","metadata":{"abstract":"The object of this,work is to, determine how the mathematical model would predict the dynamic response of a pilot plant scale distillation column under extreme transient conditions, and to demonstrate the usefulness of the model in feed-forward control of 'the column. The data from the column will be compared with the calculated results. The comparison serves as a test for the mathematical model and its computer program. The control of distillation columns has received a considerably large interest in recent years. Because the separation processes by distillation are found an almost every phase of the chemical and petroleum industries. In order to ensure smooth and economic operation of the distillation column, flows of cooling, heating media and intermediate product should be disturbed as little as possible. Thus, an accurate control of product compositions and column performance is very important. A computer program· is developed for dynamic simulation of the column. The nonlinear equations of the dynamic model are solved numerically. This model requires simultaneous solution of over-all material balances, heat balances, equilibrium and efficiency relationships for each plate. condenser and the reboiler of the column. The component mole balance establishes the liquid flowrate. The vapor liquid relationships establish the vapor composition where\nas the overall heat balance defines the vapor flow leaving the plate. The binary system of methanol-tertiary butyl alcohol is distilled in,twentyplate, which 10 cm internal diameter bubble cap distillation column which is made of glass.\n\nTurkish\n\nBu calışmanın amacı pilot· tesis düzeyinde gecici durum şartlarındaçalışan bir damıtma kulesinin· dinamik tepkilerinin matematiksel model ile tahminini hesaplamaktır. Bir ikinci amacı da bu modelin ileri-beslemeli kule kontrolündak faydasını saptamaktır. Bu amaç için bir damitma kulesinde elde edilen veriler matematiksel model icin yazılan bilgisayar programı sonuclarıyla karılaştırılmıştır. Damıtma kulelerinin koritrolu son yıllarda büyük önem kazanmıştır. Çünkü damıtma ile ayırma işlemleri bütün kimya ve petrol sanayiinde geniş bir şekilde kullanılmaktadır. Damıtma kulelerinin düzenli ve ekonomik calışmaları için soğutma ve ısıtma ayrıca ara ürünlerinin sıcaklığı ve derişimlerinin öngörülen belli sınırlar içinde kalması gerekir. Bu nedenle damıtma kulelerinin iyi bir şekilde kontrol edilmesi önemlidir. Damıtma kulesinin çalışması hakkındaki dinamik model icin bir bilgisayar programı yazılmıştır. Bu·programdaki doğrusal olmayan denklemler nümerik metodla çözülmüştür. Bu cözümde her bir tepsi ve yoğuşturucu ile kazan için genel madde denkliği, ısı denkliği ve verim bağıntıları yer almaktadır. Sıvı akım hızları her bir bileşen için yazılan molar denkliklerle bulunmuştur. Buhar deişimleri buhar-sıvı denge bağıntısıyla, bir tepsiyi terkesen buharın hızıda genel ısı denkliğiyle bulunmuştur. Bu çalışmada deneysel veriler methanol-tersiyer bütül alkol karışımı ile, 10 cm çapındaki yirmi tepsili camdan yapılmış bir damıtma kulesinde elde edilmiştir.","more_info":"ibrahim Uslu","ai_title_tag":"Dynamic Modeling and Control of a Distillation Column"},"translated_abstract":"The object of this,work is to, determine how the mathematical model would predict the dynamic response of a pilot plant scale distillation column under extreme transient conditions, and to demonstrate the usefulness of the model in feed-forward control of 'the column. The data from the column will be compared with the calculated results. The comparison serves as a test for the mathematical model and its computer program. The control of distillation columns has received a considerably large interest in recent years. Because the separation processes by distillation are found an almost every phase of the chemical and petroleum industries. In order to ensure smooth and economic operation of the distillation column, flows of cooling, heating media and intermediate product should be disturbed as little as possible. Thus, an accurate control of product compositions and column performance is very important. A computer program· is developed for dynamic simulation of the column. The nonlinear equations of the dynamic model are solved numerically. This model requires simultaneous solution of over-all material balances, heat balances, equilibrium and efficiency relationships for each plate. condenser and the reboiler of the column. The component mole balance establishes the liquid flowrate. The vapor liquid relationships establish the vapor composition where\nas the overall heat balance defines the vapor flow leaving the plate. The binary system of methanol-tertiary butyl alcohol is distilled in,twentyplate, which 10 cm internal diameter bubble cap distillation column which is made of glass.\n\nTurkish\n\nBu calışmanın amacı pilot· tesis düzeyinde gecici durum şartlarındaçalışan bir damıtma kulesinin· dinamik tepkilerinin matematiksel model ile tahminini hesaplamaktır. Bir ikinci amacı da bu modelin ileri-beslemeli kule kontrolündak faydasını saptamaktır. Bu amaç için bir damitma kulesinde elde edilen veriler matematiksel model icin yazılan bilgisayar programı sonuclarıyla karılaştırılmıştır. Damıtma kulelerinin koritrolu son yıllarda büyük önem kazanmıştır. Çünkü damıtma ile ayırma işlemleri bütün kimya ve petrol sanayiinde geniş bir şekilde kullanılmaktadır. Damıtma kulelerinin düzenli ve ekonomik calışmaları için soğutma ve ısıtma ayrıca ara ürünlerinin sıcaklığı ve derişimlerinin öngörülen belli sınırlar içinde kalması gerekir. Bu nedenle damıtma kulelerinin iyi bir şekilde kontrol edilmesi önemlidir. Damıtma kulesinin çalışması hakkındaki dinamik model icin bir bilgisayar programı yazılmıştır. Bu·programdaki doğrusal olmayan denklemler nümerik metodla çözülmüştür. Bu cözümde her bir tepsi ve yoğuşturucu ile kazan için genel madde denkliği, ısı denkliği ve verim bağıntıları yer almaktadır. Sıvı akım hızları her bir bileşen için yazılan molar denkliklerle bulunmuştur. Buhar deişimleri buhar-sıvı denge bağıntısıyla, bir tepsiyi terkesen buharın hızıda genel ısı denkliğiyle bulunmuştur. Bu çalışmada deneysel veriler methanol-tersiyer bütül alkol karışımı ile, 10 cm çapındaki yirmi tepsili camdan yapılmış bir damıtma kulesinde elde 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href="https://www.academia.edu/1146696/TRANFOOD_Radionuclide_Transport_via_Terrestrial_Food_Chain_I_Uslu_D_E_Fields_M_G_Yal%C3%A7%C4%B1nta%C5%9F_1988_USA_Oak_Ridge_National_Laboratory"><img alt="Research paper thumbnail of TRANFOOD Radionuclide Transport via Terrestrial Food Chain , I. Uslu, D. E. Fields. M. G. Yalçıntaş. (1988), USA, Oak Ridge National Laboratory" class="work-thumbnail" src="https://attachments.academia-assets.com/7377304/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1146696/TRANFOOD_Radionuclide_Transport_via_Terrestrial_Food_Chain_I_Uslu_D_E_Fields_M_G_Yal%C3%A7%C4%B1nta%C5%9F_1988_USA_Oak_Ridge_National_Laboratory">TRANFOOD Radionuclide Transport via Terrestrial Food Chain , I. Uslu, D. E. Fields. M. G. Yalçıntaş. (1988), USA, Oak Ridge National Laboratory</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A dynamic, time-dependent model has been developed for simulation of an acute environmental trans...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A dynamic, time-dependent model has been developed for simulation of an acute environmental transfer of radionuclides through agricultural systems. TRANFOOD is a computer code which calculates concentration of radionuclides in surface and root-zone soil, deep soil, produce and feed, and beef and milk from a given initial surface concentration of radioactivity from fallout. The preliminary validation of the model was carried out by comparing the results with Chernobyl Nuclear Accident data of the Federal Republic of Germany. The measured and calculated results are in agreement, inasmuch as nearly the same amount of peak specific activities were seen, but there is a sharp reduction of measured specific activity values for both /sup 137/Cs and /sup 131/I after May 5, 1986. The differences in observed and simulated values for this period is likely due to some protective actions which had been taken in the Federal Republic of Germany. Amerika Birleşik Devletleri . Oak Ridge National Laboratory.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2443e733175ed89d177ae2206ed1d8f1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7377304,&quot;asset_id&quot;:1146696,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7377304/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1146696"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1146696"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1146696; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1146696]").text(description); $(".js-view-count[data-work-id=1146696]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1146696; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1146696']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1146696, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "2443e733175ed89d177ae2206ed1d8f1" } } $('.js-work-strip[data-work-id=1146696]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1146696,"title":"TRANFOOD Radionuclide Transport via Terrestrial Food Chain , I. 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data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1204252/Categorization_of_Radioactive_Sources"><img alt="Research paper thumbnail of Categorization of Radioactive Sources" class="work-thumbnail" src="https://attachments.academia-assets.com/7475329/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1204252/Categorization_of_Radioactive_Sources">Categorization of Radioactive Sources</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The objective of this Safety Guide is to provide a simple, logical system for ranking radioactive...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The objective of this Safety Guide is to provide a simple, logical system for ranking radioactive sources in terms of their potential to cause harm to human health, and for grouping sources and the practices in which they are used into discrete categories. This categorization can assist regulatory bodies in establishing regulatory requirements that ensure an appropriate level of<br />control for each authorized source.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="54f61591b2744f8cd71896cb1d630189" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7475329,&quot;asset_id&quot;:1204252,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7475329/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1204252"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1204252"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1204252; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1204252]").text(description); $(".js-view-count[data-work-id=1204252]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1204252; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1204252']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1204252, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "54f61591b2744f8cd71896cb1d630189" } } $('.js-work-strip[data-work-id=1204252]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1204252,"title":"Categorization of Radioactive Sources","translated_title":"","metadata":{"abstract":"The objective of this Safety Guide is to provide a simple, logical system for ranking radioactive sources in terms of their potential to cause harm to human health, and for grouping sources and the practices in which they are used into discrete categories. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1204224"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1204224/Safety_considerations_in_the_disposal_of_disused_sealed_radioactive_sources_in_borehole_facilities"><img alt="Research paper thumbnail of Safety considerations in the disposal of disused sealed radioactive sources in borehole facilities" class="work-thumbnail" src="https://attachments.academia-assets.com/7475271/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1204224/Safety_considerations_in_the_disposal_of_disused_sealed_radioactive_sources_in_borehole_facilities">Safety considerations in the disposal of disused sealed radioactive sources in borehole facilities</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The objective of this report is to address safety issues relevant to the disposal of disused seal...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The objective of this report is to address safety issues relevant to the disposal of disused sealed sources, and other limited amounts of radioactive waste, in borehole facilities. It is the first in a series of reports aiming to provide an indication of the present issues related to the use of borehole disposal facilities to safely disposal of disused sealed radioactive sources and other smaller quantities of radioactive waste and to identify areas were further work needs to be undertaken.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="450cd2b5107e3d84dcfbf69074738653" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7475271,&quot;asset_id&quot;:1204224,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7475271/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1204224"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1204224"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1204224; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1204224]").text(description); $(".js-view-count[data-work-id=1204224]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1204224; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1204224']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1204224, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "450cd2b5107e3d84dcfbf69074738653" } } $('.js-work-strip[data-work-id=1204224]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1204224,"title":"Safety considerations in the disposal of disused sealed radioactive sources in borehole facilities","translated_title":"","metadata":{"abstract":"The objective of this report is to address safety issues relevant to the disposal of disused sealed sources, and other limited amounts of radioactive waste, in borehole facilities. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1189790"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1189790/The_Production_Characterization_and_Burnup_up_of_urani%C4%B1m_Dioxide_Gadolinium_Oxide_Fuel_and_Boron_Nitride_Coated_Uranium_Dioxide_Gadolinium_Oxide_Fuel"><img alt="Research paper thumbnail of The Production, Characterization and Burnup up of uraniım Dioxide-Gadolinium Oxide Fuel and Boron Nitride Coated Uranium Dioxide-Gadolinium Oxide Fuel" class="work-thumbnail" src="https://attachments.academia-assets.com/7376730/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1189790/The_Production_Characterization_and_Burnup_up_of_urani%C4%B1m_Dioxide_Gadolinium_Oxide_Fuel_and_Boron_Nitride_Coated_Uranium_Dioxide_Gadolinium_Oxide_Fuel">The Production, Characterization and Burnup up of uraniım Dioxide-Gadolinium Oxide Fuel and Boron Nitride Coated Uranium Dioxide-Gadolinium Oxide Fuel</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this research work pure urania and urania-gadolonia (5 and 10%) fuels were first produced by s...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this research work pure urania and urania-gadolonia (5 and 10%) fuels were first produced by sol-gel technique. The effects of some operational parameters such as grinding, use of binder, compaction pressure, and reduction temperature on the porosity of the sintered fuels were investigated. The sintered fuel pellets were then coated with boron nitride (BN). This is achieved through chemcial vapor depositon (CVD) using boron tricholoride and ammonia. The coated samples were sintered at 1600 K. The burn up calculations by using WİMS-D/4 showed that boron nitride coated and gadolinia containing fuels had larger burnups than other fuels. The calculations were repeated at different pitch distances. The change of radius of the fuel pellet ot the moderator/fuel ratio did not introduce an improvement in the performance of fuel and all fuel gives the highest burnup at the present design values of a PWR.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6cb5971212e6459ee94ba3b9be8a8c27" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7376730,&quot;asset_id&quot;:1189790,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7376730/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1189790"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1189790"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1189790; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1189790]").text(description); $(".js-view-count[data-work-id=1189790]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1189790; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1189790']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1189790, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "6cb5971212e6459ee94ba3b9be8a8c27" } } $('.js-work-strip[data-work-id=1189790]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1189790,"title":"The Production, Characterization and Burnup up of uraniım Dioxide-Gadolinium Oxide Fuel and Boron Nitride Coated Uranium Dioxide-Gadolinium Oxide Fuel","translated_title":"","metadata":{"abstract":"In this research work pure urania and urania-gadolonia (5 and 10%) fuels were first produced by sol-gel technique. 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thumbnail of Nükleer Güç Santrallarında Toryum Kullanımı" class="work-thumbnail" src="https://attachments.academia-assets.com/7376622/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1191424/N%C3%BCkleer_G%C3%BC%C3%A7_Santrallar%C4%B1nda_Toryum_Kullan%C4%B1m%C4%B1">Nükleer Güç Santrallarında Toryum Kullanımı</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bir ön çalışma niteliği taşıyan bu çalışma ile toryum yakıt çevrimi ve Türkiye açısından önemi vu...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bir ön çalışma niteliği taşıyan bu çalışma ile toryum yakıt çevrimi ve Türkiye açısından önemi vurgulanmak istenmiştir. Bu çalışmanın temel amacı Dünyanın torym kaynaklarının %20 sinden fazlasına sahip ülkemizin uranyum yakıt çevrimine alternatif olarak toryum yakıt çevrimine araştırma ve geliştirme çalışmalarında daha fazla yer verilmesi gereğine dikkat çekmektir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ebc5028a47962ba86a06a60f00453b26" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7376622,&quot;asset_id&quot;:1191424,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7376622/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1191424"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1191424"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1191424; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1191424]").text(description); $(".js-view-count[data-work-id=1191424]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1191424; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1191424']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1191424, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "ebc5028a47962ba86a06a60f00453b26" } } $('.js-work-strip[data-work-id=1191424]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1191424,"title":"Nükleer Güç Santrallarında Toryum Kullanımı","translated_title":"","metadata":{"abstract":"Bir ön çalışma niteliği taşıyan bu çalışma ile toryum yakıt çevrimi ve Türkiye açısından önemi vurgulanmak istenmiştir. 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Inside the fence, gamma exposure rates above background levels were identified at 98 areas totaling -800 m2. Of most immediate concern was a 38-m2 area by the south fence that had gamma exposure rates of<br />1 mR/h at 1 m above the ground surface and 10 mR/h at the surface. Beta activity was detected in the leaves of several small saplings growing in this area, and some spillover of contaminated leaves outside the fence was evident. Other elevated areas inside the fence ranged from 17 pR/h to 1400 pR/h, except for seven scattered spots that had readings of 2 or 3 mR/h: No contamination was found outside the fence on the west, south, and east sides. Three areas of contamination ranging from 17 to 340 pR/h were defined outside the fence on the north side.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="3fec58302af19903110594d9d1bd97cf" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:11402937,&quot;asset_id&quot;:1460323,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/11402937/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1460323"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1460323"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1460323; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1460323]").text(description); $(".js-view-count[data-work-id=1460323]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1460323; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1460323']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1460323, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "3fec58302af19903110594d9d1bd97cf" } } $('.js-work-strip[data-work-id=1460323]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1460323,"title":"SURFACE RADIOLOGCCAL INVESTIGATIQNS AT SOLID WASTE STORAGE","translated_title":"","metadata":{"abstract":"Solid Waste Storage Area 3 (SWSA 3), located in a fenced area 1 km west of the west entrance to Oak Ridge National Laboratory (ORNL), was surveyed to determine the level and extent of surface radiological contamination. Inside the fence, gamma exposure rates above background levels were identified at 98 areas totaling -800 m2. Of most immediate concern was a 38-m2 area by the south fence that had gamma exposure rates of\n1 mR/h at 1 m above the ground surface and 10 mR/h at the surface. Beta activity was detected in the leaves of several small saplings growing in this area, and some spillover of contaminated leaves outside the fence was evident. Other elevated areas inside the fence ranged from 17 pR/h to 1400 pR/h, except for seven scattered spots that had readings of 2 or 3 mR/h: No contamination was found outside the fence on the west, south, and east sides. Three areas of contamination ranging from 17 to 340 pR/h were defined outside the fence on the north side.","more_info":"M. S. Uziel, J. A. Roberts, J. K. Williams\nOAK RIDGE NATIONAL LABORATORY\nORNL/RAP/LTR-88/\nFebruary 1, 1988\n\nI am contibuted to this book as a Survey Team Member. \nB. A. Berven, N. Ozluoglu, A. C. Butler, W. D. Cottrell, I. Uslu, D. E. Fields\nS. D. Jones, W. Winton, J. E. Nyquist, D. A. Roberts, J. K. Williams, M. G. Yalcintas are the survey team members of this study."},"translated_abstract":"Solid Waste Storage Area 3 (SWSA 3), located in a fenced area 1 km west of the west entrance to Oak Ridge National Laboratory (ORNL), was surveyed to determine the level and extent of surface radiological contamination. Inside the fence, gamma exposure rates above background levels were identified at 98 areas totaling -800 m2. Of most immediate concern was a 38-m2 area by the south fence that had gamma exposure rates of\n1 mR/h at 1 m above the ground surface and 10 mR/h at the surface. Beta activity was detected in the leaves of several small saplings growing in this area, and some spillover of contaminated leaves outside the fence was evident. Other elevated areas inside the fence ranged from 17 pR/h to 1400 pR/h, except for seven scattered spots that had readings of 2 or 3 mR/h: No contamination was found outside the fence on the west, south, and east sides. Three areas of contamination ranging from 17 to 340 pR/h were defined outside the fence on the north side.","internal_url":"https://www.academia.edu/1460323/SURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_SOLID_WASTE_STORAGE","translated_internal_url":"","created_at":"2012-03-04T05:53:46.100-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"book","co_author_tags":[],"downloadable_attachments":[{"id":11402937,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/11402937/thumbnails/1.jpg","file_name":"survay team member.pdf","download_url":"https://www.academia.edu/attachments/11402937/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"SURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_S.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/11402937/survay_team_member-libre.pdf?1392879733=\u0026response-content-disposition=attachment%3B+filename%3DSURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_S.pdf\u0026Expires=1733898196\u0026Signature=K-dGsvT5xLeuDea7qCUQl17k30XbgOT4mCOBFnESIX6AGyTmvm1MyY0EDJZ1ULIjMMK~JtIAqr7zaZRY4Ju9MIi9yPMSH-kG~FHZkkvPe8oKwvetiWhn3dFgNgXU7Fh1~jJ8B7Gz9Nn8P5w0uG~SRabrPj~lL~hgav3cGPdcQsVwFwWChI5~mhW-4O~F8Z9DzJT3gQRuPq7aGptO3uXz~HoE~m0lBnV2Fj8yeOZA9k3Cf5Bo76PwZgUssQVSAz8SKCR2gY5fMV9V5FNo79ig1XG5WJdJ9uHxIJGolSwguw45OmBv5xK7NFaHAX7rE~fC1IdGR6KQCltgUMGrFgkgKA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"SURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_SOLID_WASTE_STORAGE","translated_slug":"","page_count":47,"language":"en","content_type":"Work","summary":"Solid Waste Storage Area 3 (SWSA 3), located in a fenced area 1 km west of the west entrance to Oak Ridge National Laboratory (ORNL), was surveyed to determine the level and extent of surface radiological contamination. Inside the fence, gamma exposure rates above background levels were identified at 98 areas totaling -800 m2. Of most immediate concern was a 38-m2 area by the south fence that had gamma exposure rates of\n1 mR/h at 1 m above the ground surface and 10 mR/h at the surface. Beta activity was detected in the leaves of several small saplings growing in this area, and some spillover of contaminated leaves outside the fence was evident. Other elevated areas inside the fence ranged from 17 pR/h to 1400 pR/h, except for seven scattered spots that had readings of 2 or 3 mR/h: No contamination was found outside the fence on the west, south, and east sides. Three areas of contamination ranging from 17 to 340 pR/h were defined outside the fence on the north side.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":11402937,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/11402937/thumbnails/1.jpg","file_name":"survay team member.pdf","download_url":"https://www.academia.edu/attachments/11402937/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"SURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_S.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/11402937/survay_team_member-libre.pdf?1392879733=\u0026response-content-disposition=attachment%3B+filename%3DSURFACE_RADIOLOGCCAL_INVESTIGATIQNS_AT_S.pdf\u0026Expires=1733898196\u0026Signature=K-dGsvT5xLeuDea7qCUQl17k30XbgOT4mCOBFnESIX6AGyTmvm1MyY0EDJZ1ULIjMMK~JtIAqr7zaZRY4Ju9MIi9yPMSH-kG~FHZkkvPe8oKwvetiWhn3dFgNgXU7Fh1~jJ8B7Gz9Nn8P5w0uG~SRabrPj~lL~hgav3cGPdcQsVwFwWChI5~mhW-4O~F8Z9DzJT3gQRuPq7aGptO3uXz~HoE~m0lBnV2Fj8yeOZA9k3Cf5Bo76PwZgUssQVSAz8SKCR2gY5fMV9V5FNo79ig1XG5WJdJ9uHxIJGolSwguw45OmBv5xK7NFaHAX7rE~fC1IdGR6KQCltgUMGrFgkgKA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":55,"name":"Environmental Engineering","url":"https://www.academia.edu/Documents/in/Environmental_Engineering"},{"id":402,"name":"Environmental Science","url":"https://www.academia.edu/Documents/in/Environmental_Science"},{"id":1063,"name":"Environmental Education","url":"https://www.academia.edu/Documents/in/Environmental_Education"},{"id":1307,"name":"Environmental Law","url":"https://www.academia.edu/Documents/in/Environmental_Law"},{"id":3407,"name":"Environmental Studies","url":"https://www.academia.edu/Documents/in/Environmental_Studies"},{"id":4589,"name":"Environmental Planning and Design","url":"https://www.academia.edu/Documents/in/Environmental_Planning_and_Design"},{"id":7609,"name":"Environmental Management","url":"https://www.academia.edu/Documents/in/Environmental_Management"},{"id":7695,"name":"Environmental Ethics","url":"https://www.academia.edu/Documents/in/Environmental_Ethics"},{"id":9787,"name":"Environmental Policy and Governance","url":"https://www.academia.edu/Documents/in/Environmental_Policy_and_Governance"},{"id":18845,"name":"Environmental Sustainability","url":"https://www.academia.edu/Documents/in/Environmental_Sustainability"},{"id":386314,"name":"İbrahim","url":"https://www.academia.edu/Documents/in/Ibrahim"},{"id":386315,"name":"Uslu","url":"https://www.academia.edu/Documents/in/Uslu"},{"id":393490,"name":"Oak Ridge","url":"https://www.academia.edu/Documents/in/Oak_Ridge"}],"urls":[{"id":219140,"url":"http://www.ornl.gov/info/reports/1988/3445605715438.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1146676"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1146676/Radiation_Exposures_from_ceasium_Contaminated_Field"><img alt="Research paper thumbnail of Radiation Exposures from ceasium Contaminated Field" class="work-thumbnail" src="https://attachments.academia-assets.com/7384324/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1146676/Radiation_Exposures_from_ceasium_Contaminated_Field">Radiation Exposures from ceasium Contaminated Field</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A surface radiological investigation was conducted at Oak Ridge Reservations. The purpose of this...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A surface radiological investigation was conducted at Oak Ridge Reservations. The purpose of this scoping survey were to mesure current gamma exposure rate levels, to provide a radiological impact analysis for the Site, to calculate exposure rates after shielding the contaminated enclosures with soil or concrete and to recommend corrective actions to minimize exposures to general public and workers on Oak Ridge Reservations. Amerika Birleşik Devletleri. Oak Ridge National Laboratory.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="410ffb1eaf7aa8a5011548b5536d8696" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7384324,&quot;asset_id&quot;:1146676,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7384324/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1146676"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1146676"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1146676; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1146676]").text(description); $(".js-view-count[data-work-id=1146676]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1146676; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1146676']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1146676, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "410ffb1eaf7aa8a5011548b5536d8696" } } $('.js-work-strip[data-work-id=1146676]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1146676,"title":"Radiation Exposures from ceasium Contaminated Field","translated_title":"","metadata":{"abstract":"A surface radiological investigation was conducted at Oak Ridge Reservations. The purpose of this scoping survey were to mesure current gamma exposure rate levels, to provide a radiological impact analysis for the Site, to calculate exposure rates after shielding the contaminated enclosures with soil or concrete and to recommend corrective actions to minimize exposures to general public and workers on Oak Ridge Reservations. Amerika Birleşik Devletleri. Oak Ridge National Laboratory.","more_info":"ORNL/RAP-46 OakRidge National Laboratory\nSeptember 1988\nM.G. Yalçıntaş, M.S. Uziel, J.A. Roberts, ibrahim Uslu,","ai_title_tag":"Radiation Exposure Assessment at Cesium-Contaminated Site"},"translated_abstract":"A surface radiological investigation was conducted at Oak Ridge Reservations. The purpose of this scoping survey were to mesure current gamma exposure rate levels, to provide a radiological impact analysis for the Site, to calculate exposure rates after shielding the contaminated enclosures with soil or concrete and to recommend corrective actions to minimize exposures to general public and workers on Oak Ridge Reservations. Amerika Birleşik Devletleri. Oak Ridge National Laboratory.","internal_url":"https://www.academia.edu/1146676/Radiation_Exposures_from_ceasium_Contaminated_Field","translated_internal_url":"","created_at":"2011-12-09T23:35:29.067-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"book","co_author_tags":[],"downloadable_attachments":[{"id":7384324,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7384324/thumbnails/1.jpg","file_name":"a2.pdf","download_url":"https://www.academia.edu/attachments/7384324/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Radiation_Exposures_from_ceasium_Contami.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7384324/a2-libre.pdf?1390851218=\u0026response-content-disposition=attachment%3B+filename%3DRadiation_Exposures_from_ceasium_Contami.pdf\u0026Expires=1733756524\u0026Signature=AvS0EepWR9yFfeImx4O8YqSk4wGSGkcooFcMOw0qCnu6FGFUCaVcbIdBG9C-WvzaknKKP66ijcN8eYjbbw9L4c8JlL6EWhmMaVeg0Yy8mY-kmioeqpLeGeT~AmxF-DSGcAFbQyCY92y6mKMABQ3Yt5uJjaVd9ro1Edo5oeq47yp71lXq5SWQBV1J~PxSLSLM922B9UjLuPnGMO~4CLJ3GB6ALC62AlETTPYBkQdZc1-vsCmmDvLAz2aT7fKlLRWH6rwqK8P46JtPfwUbxsDj1WlvoFN71f031wsHPfOuc1jUZKN-t89QwaN7zYYplnAFEjuIU7lrFkLzUGMsV0mH-g__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Radiation_Exposures_from_ceasium_Contaminated_Field","translated_slug":"","page_count":26,"language":"en","content_type":"Work","summary":"A surface radiological investigation was conducted at Oak Ridge Reservations. The purpose of this scoping survey were to mesure current gamma exposure rate levels, to provide a radiological impact analysis for the Site, to calculate exposure rates after shielding the contaminated enclosures with soil or concrete and to recommend corrective actions to minimize exposures to general public and workers on Oak Ridge Reservations. Amerika Birleşik Devletleri. Oak Ridge National Laboratory.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7384324,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7384324/thumbnails/1.jpg","file_name":"a2.pdf","download_url":"https://www.academia.edu/attachments/7384324/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Radiation_Exposures_from_ceasium_Contami.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7384324/a2-libre.pdf?1390851218=\u0026response-content-disposition=attachment%3B+filename%3DRadiation_Exposures_from_ceasium_Contami.pdf\u0026Expires=1733756524\u0026Signature=AvS0EepWR9yFfeImx4O8YqSk4wGSGkcooFcMOw0qCnu6FGFUCaVcbIdBG9C-WvzaknKKP66ijcN8eYjbbw9L4c8JlL6EWhmMaVeg0Yy8mY-kmioeqpLeGeT~AmxF-DSGcAFbQyCY92y6mKMABQ3Yt5uJjaVd9ro1Edo5oeq47yp71lXq5SWQBV1J~PxSLSLM922B9UjLuPnGMO~4CLJ3GB6ALC62AlETTPYBkQdZc1-vsCmmDvLAz2aT7fKlLRWH6rwqK8P46JtPfwUbxsDj1WlvoFN71f031wsHPfOuc1jUZKN-t89QwaN7zYYplnAFEjuIU7lrFkLzUGMsV0mH-g__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":586,"name":"Health Sciences","url":"https://www.academia.edu/Documents/in/Health_Sciences"},{"id":18845,"name":"Environmental Sustainability","url":"https://www.academia.edu/Documents/in/Environmental_Sustainability"},{"id":217018,"name":"Workers","url":"https://www.academia.edu/Documents/in/Workers"},{"id":222437,"name":"Exposure","url":"https://www.academia.edu/Documents/in/Exposure"},{"id":393487,"name":"Uslu, Ibrahim","url":"https://www.academia.edu/Documents/in/Uslu_Ibrahim"},{"id":393490,"name":"Oak Ridge","url":"https://www.academia.edu/Documents/in/Oak_Ridge"},{"id":393492,"name":"Radiological","url":"https://www.academia.edu/Documents/in/Radiological"},{"id":393495,"name":"General Public","url":"https://www.academia.edu/Documents/in/General_Public"},{"id":393496,"name":"Radiological Impact","url":"https://www.academia.edu/Documents/in/Radiological_Impact"},{"id":393498,"name":"Corrective Actions","url":"https://www.academia.edu/Documents/in/Corrective_Actions"},{"id":393501,"name":"Oak Ridge National Laboratory","url":"https://www.academia.edu/Documents/in/Oak_Ridge_National_Laboratory"},{"id":393502,"name":"Shielding","url":"https://www.academia.edu/Documents/in/Shielding"}],"urls":[{"id":163736,"url":"http://www.hss.doe.gov/healthsafety/ohre/new/findingaids/epidemiologic/oakridge2/monitoff/4.html"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1192217"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1192217/Studies_on_Disposal_of_Low_level_Radioactive_Waste_in_Turkey"><img alt="Research paper thumbnail of Studies on Disposal of Low-level Radioactive Waste in Turkey" class="work-thumbnail" src="https://attachments.academia-assets.com/7384077/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1192217/Studies_on_Disposal_of_Low_level_Radioactive_Waste_in_Turkey">Studies on Disposal of Low-level Radioactive Waste in Turkey</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The Turkish Government is in the process of planning two nuclear reactors in Turkey. Studies have...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The Turkish Government is in the process of planning two nuclear reactors in Turkey. Studies have begun for improved control of low level wastes (LLW) in Turkey before establishment of these reactors. In this study, the PRESTO-II (Prediction of Radiation Exposures form Shallow Trench Operations) computer code is used to assess the risk associated with the shallow land disposal of low level waste (LLW) in various sites in Turkey. PRESTO-II is a computer code developed under the United States Environmental Protection Agency, Department of Energy and Nuclear Regulatory Commission funding to evaluate possible health effects from radioactive releases from shallow, radioactive waste disposal trenches and from areas contaminated with operational spillage. A preliminary simulation using the PRESTO-II computer code has been run for the site in Koteyli, Balikesir, Turkey. This example simulation was performed using the same radionuclide data set believed representative of the LLW disposal facility in Barnwell, South Carolina. Site environmental variables were selected to typify credible worst case exposure scenarios. Radionuclide inventories are primarily based on estimated waste composition rather than measured values.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4bd09277eac6e271c4c7a996a0a585ce" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7384077,&quot;asset_id&quot;:1192217,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7384077/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1192217"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1192217"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1192217; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1192217]").text(description); $(".js-view-count[data-work-id=1192217]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1192217; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1192217']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1192217, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "4bd09277eac6e271c4c7a996a0a585ce" } } $('.js-work-strip[data-work-id=1192217]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1192217,"title":"Studies on Disposal of Low-level Radioactive Waste in Turkey","translated_title":"","metadata":{"abstract":"The Turkish Government is in the process of planning two nuclear reactors in Turkey. Studies have begun for improved control of low level wastes (LLW) in Turkey before establishment of these reactors. In this study, the PRESTO-II (Prediction of Radiation Exposures form Shallow Trench Operations) computer code is used to assess the risk associated with the shallow land disposal of low level waste (LLW) in various sites in Turkey. PRESTO-II is a computer code developed under the United States Environmental Protection Agency, Department of Energy and Nuclear Regulatory Commission funding to evaluate possible health effects from radioactive releases from shallow, radioactive waste disposal trenches and from areas contaminated with operational spillage. A preliminary simulation using the PRESTO-II computer code has been run for the site in Koteyli, Balikesir, Turkey. This example simulation was performed using the same radionuclide data set believed representative of the LLW disposal facility in Barnwell, South Carolina. Site environmental variables were selected to typify credible worst case exposure scenarios. Radionuclide inventories are primarily based on estimated waste composition rather than measured values.","more_info":"ORNL/TM-10700 1989 Aug 01\nEnergy Citations Database\nİbrahim Uslu, D.E.Fields, M.G. Yalçıntaş","ai_title_tag":"Assessing Low-Level Radioactive Waste Disposal in Turkey"},"translated_abstract":"The Turkish Government is in the process of planning two nuclear reactors in Turkey. Studies have begun for improved control of low level wastes (LLW) in Turkey before establishment of these reactors. In this study, the PRESTO-II (Prediction of Radiation Exposures form Shallow Trench Operations) computer code is used to assess the risk associated with the shallow land disposal of low level waste (LLW) in various sites in Turkey. PRESTO-II is a computer code developed under the United States Environmental Protection Agency, Department of Energy and Nuclear Regulatory Commission funding to evaluate possible health effects from radioactive releases from shallow, radioactive waste disposal trenches and from areas contaminated with operational spillage. A preliminary simulation using the PRESTO-II computer code has been run for the site in Koteyli, Balikesir, Turkey. This example simulation was performed using the same radionuclide data set believed representative of the LLW disposal facility in Barnwell, South Carolina. Site environmental variables were selected to typify credible worst case exposure scenarios. Radionuclide inventories are primarily based on estimated waste composition rather than measured values.","internal_url":"https://www.academia.edu/1192217/Studies_on_Disposal_of_Low_level_Radioactive_Waste_in_Turkey","translated_internal_url":"","created_at":"2012-01-01T18:35:24.241-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"book","co_author_tags":[],"downloadable_attachments":[{"id":7384077,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7384077/thumbnails/1.jpg","file_name":"a1.pdf","download_url":"https://www.academia.edu/attachments/7384077/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Studies_on_Disposal_of_Low_level_Radioac.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7384077/a1-libre.pdf?1390851245=\u0026response-content-disposition=attachment%3B+filename%3DStudies_on_Disposal_of_Low_level_Radioac.pdf\u0026Expires=1733898196\u0026Signature=Dh1tUanftRrstvjVknvXGilFBNChE1~qoQzq-QPt90COOsy8JDrUzcUOkSSedLlBiQKV0O~7XLOsBCtdc~tz~ngzefxxfv0D3a1m8TGNrjsRIEkH211qrq190ryfKwuhSVQCpgCxba1vK6eC1ntPfHSppnzKpWuWVNvt4GuUz5GXzjDg9EGqo6vg-~nC8aqFmtiN4m3qtKXSZni4-Xb8hq~AEyp-7lAhSxhJjhgZ3zleoq6TKI07vA~tBFF1z4Mbfj-U4VQqtm9PgeknXOiVEb0~61J6yfJIBt~4k61PCSgLiJc9GrpfwNoGDUPZL8aAFYYWj93s1VN6jmYBqjOcDg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Studies_on_Disposal_of_Low_level_Radioactive_Waste_in_Turkey","translated_slug":"","page_count":22,"language":"en","content_type":"Work","summary":"The Turkish Government is in the process of planning two nuclear reactors in Turkey. Studies have begun for improved control of low level wastes (LLW) in Turkey before establishment of these reactors. In this study, the PRESTO-II (Prediction of Radiation Exposures form Shallow Trench Operations) computer code is used to assess the risk associated with the shallow land disposal of low level waste (LLW) in various sites in Turkey. PRESTO-II is a computer code developed under the United States Environmental Protection Agency, Department of Energy and Nuclear Regulatory Commission funding to evaluate possible health effects from radioactive releases from shallow, radioactive waste disposal trenches and from areas contaminated with operational spillage. A preliminary simulation using the PRESTO-II computer code has been run for the site in Koteyli, Balikesir, Turkey. This example simulation was performed using the same radionuclide data set believed representative of the LLW disposal facility in Barnwell, South Carolina. Site environmental variables were selected to typify credible worst case exposure scenarios. Radionuclide inventories are primarily based on estimated waste composition rather than measured values.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7384077,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7384077/thumbnails/1.jpg","file_name":"a1.pdf","download_url":"https://www.academia.edu/attachments/7384077/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Studies_on_Disposal_of_Low_level_Radioac.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7384077/a1-libre.pdf?1390851245=\u0026response-content-disposition=attachment%3B+filename%3DStudies_on_Disposal_of_Low_level_Radioac.pdf\u0026Expires=1733898196\u0026Signature=Dh1tUanftRrstvjVknvXGilFBNChE1~qoQzq-QPt90COOsy8JDrUzcUOkSSedLlBiQKV0O~7XLOsBCtdc~tz~ngzefxxfv0D3a1m8TGNrjsRIEkH211qrq190ryfKwuhSVQCpgCxba1vK6eC1ntPfHSppnzKpWuWVNvt4GuUz5GXzjDg9EGqo6vg-~nC8aqFmtiN4m3qtKXSZni4-Xb8hq~AEyp-7lAhSxhJjhgZ3zleoq6TKI07vA~tBFF1z4Mbfj-U4VQqtm9PgeknXOiVEb0~61J6yfJIBt~4k61PCSgLiJc9GrpfwNoGDUPZL8aAFYYWj93s1VN6jmYBqjOcDg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":58819,"name":"Radioactive waste management","url":"https://www.academia.edu/Documents/in/Radioactive_waste_management"},{"id":386314,"name":"İbrahim","url":"https://www.academia.edu/Documents/in/Ibrahim"},{"id":386315,"name":"Uslu","url":"https://www.academia.edu/Documents/in/Uslu"},{"id":395845,"name":"Low Level Wastes","url":"https://www.academia.edu/Documents/in/Low_Level_Wastes"},{"id":395847,"name":"Computer Code","url":"https://www.academia.edu/Documents/in/Computer_Code"}],"urls":[{"id":172076,"url":"http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=5947773"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="162183" id="talks"><div class="js-work-strip profile--work_container" data-work-id="1757661"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/1757661/Dielectric_Properties_of_Electrospun_Nanofibers_PVA_PVP_and_Their_Mixtures"><img alt="Research paper thumbnail of Dielectric Properties of Electrospun Nanofibers PVA, PVP and Their Mixtures" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/1757661/Dielectric_Properties_of_Electrospun_Nanofibers_PVA_PVP_and_Their_Mixtures">Dielectric Properties of Electrospun Nanofibers PVA, PVP and Their Mixtures</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP) polymers are commonly used solvents for p...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP) polymers are commonly used solvents for producing nanofibers by Electrospinning method. Dielectric properties of PVP, PVA and their blends that are prepared by electrospinning were determined as a function of concentration in order to explore the possibility of using them as dielectric materials in different industrial applications. For this purpose, electrospun nanofibers are pressed into pellets with a hydraulic press. These samples of nanofibers were placed between two parallel Au electrode plates to read the admittance values of them. Measuremets were performed at 1 kHz - 13 MHz frequency range and at room temperature. The characterizations of nanofibers were carried out by a scanning electron microscope (SEM) and Fourier transform infrared spectroscopy (FTIR). It was discussed how to change the dielectric properties by mixing PVP.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1757661"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1757661"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1757661; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1757661]").text(description); $(".js-view-count[data-work-id=1757661]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1757661; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1757661']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1757661, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=1757661]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1757661,"title":"Dielectric Properties of Electrospun Nanofibers PVA, PVP and Their Mixtures","translated_title":"","metadata":{"abstract":"Polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP) polymers are commonly used solvents for producing nanofibers by Electrospinning method. Dielectric properties of PVP, PVA and their blends that are prepared by electrospinning were determined as a function of concentration in order to explore the possibility of using them as dielectric materials in different industrial applications. For this purpose, electrospun nanofibers are pressed into pellets with a hydraulic press. These samples of nanofibers were placed between two parallel Au electrode plates to read the admittance values of them. Measuremets were performed at 1 kHz - 13 MHz frequency range and at room temperature. The characterizations of nanofibers were carried out by a scanning electron microscope (SEM) and Fourier transform infrared spectroscopy (FTIR). It was discussed how to change the dielectric properties by mixing PVP.","more_info":"Haziret Durmuş, Mehmet Okan Erdal, Mustafa Koyuncu, Abdullah Deryal, İbrahim Uslu\u000b\nPoster sunum\n8. Nanoscience and Nanotechnolgy Congress \n(VIII. Türkiye Nanobilim - Nanoteknoloji Kongresi) \nHacettepe University, Ankara, 25-28 July, 2012","conference_end_date":{"day":28,"month":6,"year":2012,"errors":{}},"conference_start_date":{"day":25,"month":6,"year":2012,"errors":{}}},"translated_abstract":"Polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP) polymers are commonly used solvents for producing nanofibers by Electrospinning method. Dielectric properties of PVP, PVA and their blends that are prepared by electrospinning were determined as a function of concentration in order to explore the possibility of using them as dielectric materials in different industrial applications. For this purpose, electrospun nanofibers are pressed into pellets with a hydraulic press. These samples of nanofibers were placed between two parallel Au electrode plates to read the admittance values of them. Measuremets were performed at 1 kHz - 13 MHz frequency range and at room temperature. The characterizations of nanofibers were carried out by a scanning electron microscope (SEM) and Fourier transform infrared spectroscopy (FTIR). It was discussed how to change the dielectric properties by mixing PVP.","internal_url":"https://www.academia.edu/1757661/Dielectric_Properties_of_Electrospun_Nanofibers_PVA_PVP_and_Their_Mixtures","translated_internal_url":"","created_at":"2012-07-01T22:14:25.167-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[],"slug":"Dielectric_Properties_of_Electrospun_Nanofibers_PVA_PVP_and_Their_Mixtures","translated_slug":"","page_count":null,"language":"en","content_type":"Work","summary":"Polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP) polymers are commonly used solvents for producing nanofibers by Electrospinning method. Dielectric properties of PVP, PVA and their blends that are prepared by electrospinning were determined as a function of concentration in order to explore the possibility of using them as dielectric materials in different industrial applications. For this purpose, electrospun nanofibers are pressed into pellets with a hydraulic press. These samples of nanofibers were placed between two parallel Au electrode plates to read the admittance values of them. Measuremets were performed at 1 kHz - 13 MHz frequency range and at room temperature. The characterizations of nanofibers were carried out by a scanning electron microscope (SEM) and Fourier transform infrared spectroscopy (FTIR). It was discussed how to change the dielectric properties by mixing PVP.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1757524"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1757524/Antibacterial_wound_dressing_material_with_aloe_vera"><img alt="Research paper thumbnail of Antibacterial wound dressing material with aloe vera" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1757524/Antibacterial_wound_dressing_material_with_aloe_vera">Antibacterial wound dressing material with aloe vera</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The aim of the present work is to develop wound dressings which are innovative in terms of the wo...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The aim of the present work is to develop wound dressings which are innovative in terms of the wound healing rate and performance. The incorporation of drugs into the dressings make these dressings antimicrobial and help in control of infection around the wound. We have designed and developed wound dressing materials based on PVA/PAA, ciprofloxacin and aloe vera so that the wound undergoes proper healing where scar formation is the minimum. FT-IR analysis revealed that all characteristics and diameters of nanofibers was observed with SEM images.<br />The goal of this study is to produce wound dressing materials which prevent adherence of microorganism and provide quick wound healing. In terms of efficient use a wound dressing material it should have oxygen and humidity permeability by means of porous or fibrous structure and release drug for wide range area. It&#39;s possible to produce a material which has all of these properties by using nanotechnological methods. These type of materials can be produced via electro spinning technique. Poly(vinyl alcohol) (PVA) and Poly(acrylic acid) (PAA) have been frequently used in the preparation of various membranes due to their good biocompatibility and high swelling capability coupled with relatively good mechanical properties [1]. Ciprofloxacin is a broad spectrum antibiotic and has been used as component of wound dressings [2]. Aloe vera whose therapeutic effect is known for many years was added in order to provide quick wound healing. In this study ciprofloxacin and aloe vera was added one by one and together to observe differences between them. The fibrous wound dressing materials were prepared by the use of electro spinning technique. The electro spinning equipment uses a variable high voltage power supply from Gamma High Voltage Research (USA) [3]. The syringe needle was used as the electrode connected to the power source. The following operative parameters were chosen: a flow rate of 0.8 ml/h and an applied voltage of 15 kV [4]. Finally nanofibers were detached from Al foil collector and dried in the furnace at 80 °C overnight under vacuum [5]. Obtained nanofibers was characterized using SEM (Scanning Electron Microscopy) and FT-IR (Fourier transform infrared spectroscopy). SEM images show that, adding aloe vera makes nanofibers stronger and more linear than the others. FT-IR graphic show one another link up substances present of nanofibers and enable to investigate the structure of produced substance. <br />Release of ciprofloxacin was measured in ciprofloxacin and aloe vera doped nanofibers. In releasing experiment Pseudomonas aeruginosa and Staphylococcus aureus bacteria were used. Bacteria were inoculated to their suitable mediums. Then nanofibers were placed on medium with bacteria. Release ciprofloxacin from nanofiber prevent the bacterium growth and a clear zone occurs around nanofiber. Zone diameter around ciprofloxacin doped nanofibers is about 6 cm, zone diameter around ciprofloxacin and aloe vera doped nanofibers is about 5.5 cm. This shows that, when aloe vera added, ciprofloxacin slightly decrease it’s activity. According to adherence tests, electrospun nanofiber sample which contains aloe vera and ciprofloxacin has the least bacterial adherences. The highest bacterial adherence was observed at the sample which has no aloe vera and ciprofloxacin.<br /><br />*Corresponding author: <a href="mailto:h_serincay@hotmail.com" rel="nofollow">h_serincay@hotmail.com</a><br />[1] H. Bodugöz et al., O. Radiat. Phys. Chem. 55, 667, (1999).<br />[2] S. Çalangu, Klimik Dergisi 3, 115, 1990.<br />[3] I. Uslu and A. Aytimur, J. Appl. Polym. Sci. DOI: 10.1002/app.35525<br />[4] I.Uslu et al., Hacettepe J. Biol. Chem, 38, 19, (2009).<br />[5] I. Uslu et al., Hacettepe J. Biol. Chem, 36, 117, (2008).</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e2a0353708beaa8481d486ead999d6e1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:21899442,&quot;asset_id&quot;:1757524,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/21899442/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1757524"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1757524"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1757524; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1757524]").text(description); $(".js-view-count[data-work-id=1757524]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1757524; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1757524']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1757524, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "e2a0353708beaa8481d486ead999d6e1" } } $('.js-work-strip[data-work-id=1757524]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1757524,"title":"Antibacterial wound dressing material with aloe vera","translated_title":"","metadata":{"abstract":"The aim of the present work is to develop wound dressings which are innovative in terms of the wound healing rate and performance. The incorporation of drugs into the dressings make these dressings antimicrobial and help in control of infection around the wound. We have designed and developed wound dressing materials based on PVA/PAA, ciprofloxacin and aloe vera so that the wound undergoes proper healing where scar formation is the minimum. FT-IR analysis revealed that all characteristics and diameters of nanofibers was observed with SEM images.\nThe goal of this study is to produce wound dressing materials which prevent adherence of microorganism and provide quick wound healing. In terms of efficient use a wound dressing material it should have oxygen and humidity permeability by means of porous or fibrous structure and release drug for wide range area. It's possible to produce a material which has all of these properties by using nanotechnological methods. These type of materials can be produced via electro spinning technique. Poly(vinyl alcohol) (PVA) and Poly(acrylic acid) (PAA) have been frequently used in the preparation of various membranes due to their good biocompatibility and high swelling capability coupled with relatively good mechanical properties [1]. Ciprofloxacin is a broad spectrum antibiotic and has been used as component of wound dressings [2]. Aloe vera whose therapeutic effect is known for many years was added in order to provide quick wound healing. In this study ciprofloxacin and aloe vera was added one by one and together to observe differences between them. The fibrous wound dressing materials were prepared by the use of electro spinning technique. The electro spinning equipment uses a variable high voltage power supply from Gamma High Voltage Research (USA) [3]. The syringe needle was used as the electrode connected to the power source. The following operative parameters were chosen: a flow rate of 0.8 ml/h and an applied voltage of 15 kV [4]. Finally nanofibers were detached from Al foil collector and dried in the furnace at 80 °C overnight under vacuum [5]. Obtained nanofibers was characterized using SEM (Scanning Electron Microscopy) and FT-IR (Fourier transform infrared spectroscopy). SEM images show that, adding aloe vera makes nanofibers stronger and more linear than the others. FT-IR graphic show one another link up substances present of nanofibers and enable to investigate the structure of produced substance. \nRelease of ciprofloxacin was measured in ciprofloxacin and aloe vera doped nanofibers. In releasing experiment Pseudomonas aeruginosa and Staphylococcus aureus bacteria were used. Bacteria were inoculated to their suitable mediums. Then nanofibers were placed on medium with bacteria. Release ciprofloxacin from nanofiber prevent the bacterium growth and a clear zone occurs around nanofiber. Zone diameter around ciprofloxacin doped nanofibers is about 6 cm, zone diameter around ciprofloxacin and aloe vera doped nanofibers is about 5.5 cm. This shows that, when aloe vera added, ciprofloxacin slightly decrease it’s activity. According to adherence tests, electrospun nanofiber sample which contains aloe vera and ciprofloxacin has the least bacterial adherences. The highest bacterial adherence was observed at the sample which has no aloe vera and ciprofloxacin.\n\n*Corresponding author: h_serincay@hotmail.com\n[1] H. Bodugöz et al., O. Radiat. Phys. Chem. 55, 667, (1999).\n[2] S. Çalangu, Klimik Dergisi 3, 115, 1990.\n[3] I. Uslu and A. Aytimur, J. Appl. Polym. Sci. DOI: 10.1002/app.35525\n[4] I.Uslu et al., Hacettepe J. Biol. Chem, 38, 19, (2009).\n[5] I. Uslu et al., Hacettepe J. Biol. Chem, 36, 117, (2008).","more_info":"Halime Serinçay, Semiha Özkan, İbrahim USLU, Serhat Koçyiğit\nSözlü Sunum\n8. Nanoscience and Nanotechnolgy Congress (VIII. Türkiye Nanobilim - Nanoteknoloji Kongresi) Hacettepe University, Ankara, 25-28 July, 2012","conference_end_date":{"day":28,"month":6,"year":2012,"errors":{}},"conference_start_date":{"day":25,"month":6,"year":2012,"errors":{}}},"translated_abstract":"The aim of the present work is to develop wound dressings which are innovative in terms of the wound healing rate and performance. The incorporation of drugs into the dressings make these dressings antimicrobial and help in control of infection around the wound. We have designed and developed wound dressing materials based on PVA/PAA, ciprofloxacin and aloe vera so that the wound undergoes proper healing where scar formation is the minimum. FT-IR analysis revealed that all characteristics and diameters of nanofibers was observed with SEM images.\nThe goal of this study is to produce wound dressing materials which prevent adherence of microorganism and provide quick wound healing. In terms of efficient use a wound dressing material it should have oxygen and humidity permeability by means of porous or fibrous structure and release drug for wide range area. It's possible to produce a material which has all of these properties by using nanotechnological methods. These type of materials can be produced via electro spinning technique. Poly(vinyl alcohol) (PVA) and Poly(acrylic acid) (PAA) have been frequently used in the preparation of various membranes due to their good biocompatibility and high swelling capability coupled with relatively good mechanical properties [1]. Ciprofloxacin is a broad spectrum antibiotic and has been used as component of wound dressings [2]. Aloe vera whose therapeutic effect is known for many years was added in order to provide quick wound healing. In this study ciprofloxacin and aloe vera was added one by one and together to observe differences between them. The fibrous wound dressing materials were prepared by the use of electro spinning technique. The electro spinning equipment uses a variable high voltage power supply from Gamma High Voltage Research (USA) [3]. The syringe needle was used as the electrode connected to the power source. The following operative parameters were chosen: a flow rate of 0.8 ml/h and an applied voltage of 15 kV [4]. Finally nanofibers were detached from Al foil collector and dried in the furnace at 80 °C overnight under vacuum [5]. Obtained nanofibers was characterized using SEM (Scanning Electron Microscopy) and FT-IR (Fourier transform infrared spectroscopy). SEM images show that, adding aloe vera makes nanofibers stronger and more linear than the others. FT-IR graphic show one another link up substances present of nanofibers and enable to investigate the structure of produced substance. \nRelease of ciprofloxacin was measured in ciprofloxacin and aloe vera doped nanofibers. In releasing experiment Pseudomonas aeruginosa and Staphylococcus aureus bacteria were used. Bacteria were inoculated to their suitable mediums. Then nanofibers were placed on medium with bacteria. Release ciprofloxacin from nanofiber prevent the bacterium growth and a clear zone occurs around nanofiber. Zone diameter around ciprofloxacin doped nanofibers is about 6 cm, zone diameter around ciprofloxacin and aloe vera doped nanofibers is about 5.5 cm. This shows that, when aloe vera added, ciprofloxacin slightly decrease it’s activity. According to adherence tests, electrospun nanofiber sample which contains aloe vera and ciprofloxacin has the least bacterial adherences. The highest bacterial adherence was observed at the sample which has no aloe vera and ciprofloxacin.\n\n*Corresponding author: h_serincay@hotmail.com\n[1] H. Bodugöz et al., O. Radiat. Phys. Chem. 55, 667, (1999).\n[2] S. Çalangu, Klimik Dergisi 3, 115, 1990.\n[3] I. Uslu and A. Aytimur, J. Appl. Polym. Sci. DOI: 10.1002/app.35525\n[4] I.Uslu et al., Hacettepe J. Biol. Chem, 38, 19, (2009).\n[5] I. Uslu et al., Hacettepe J. Biol. Chem, 36, 117, (2008).","internal_url":"https://www.academia.edu/1757524/Antibacterial_wound_dressing_material_with_aloe_vera","translated_internal_url":"","created_at":"2012-07-01T20:36:54.908-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":21899442,"title":"","file_type":"ppt","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"halime_nano.ppt","download_url":"https://www.academia.edu/attachments/21899442/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Antibacterial_wound_dressing_material_wi.ppt","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/21899442/halime_nano.ppt?1341200129=\u0026response-content-disposition=attachment%3B+filename%3DAntibacterial_wound_dressing_material_wi.ppt\u0026Expires=1731454491\u0026Signature=LfL-QzMJhTAlFXyrvctx-5D4PtwXCHsoFeM0cxy4r4-ZFRpTS46QtylXdKCOloEfyXUGGVP03Q5D1FaIhaxCBalbc51Zip~pTMJzI7CUkzSx1D45wPCqFc9w7tNLRZVfbmtD57M2KR~CZL4VYErBoYndNi1ANfwZqP5NnLQa-7Pa8bSsToMCZCBl99LQU~In0Xx9mioVMx8oCKuXR7JklbzgfTqDBEDtVOuYBZ-wEU0hcuxO771-zJDHDp9eTKTHI5yt63tmumHD4Rs-zZqVF23COLkU21SGJwYeprJ-gk93ohYbteqaw7l8vGG3Gsed2p-Ffcd8pgvv5aR0TITrNg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Antibacterial_wound_dressing_material_with_aloe_vera","translated_slug":"","page_count":45,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":21899442,"title":"","file_type":"ppt","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"halime_nano.ppt","download_url":"https://www.academia.edu/attachments/21899442/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Antibacterial_wound_dressing_material_wi.ppt","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/21899442/halime_nano.ppt?1341200129=\u0026response-content-disposition=attachment%3B+filename%3DAntibacterial_wound_dressing_material_wi.ppt\u0026Expires=1731454491\u0026Signature=LfL-QzMJhTAlFXyrvctx-5D4PtwXCHsoFeM0cxy4r4-ZFRpTS46QtylXdKCOloEfyXUGGVP03Q5D1FaIhaxCBalbc51Zip~pTMJzI7CUkzSx1D45wPCqFc9w7tNLRZVfbmtD57M2KR~CZL4VYErBoYndNi1ANfwZqP5NnLQa-7Pa8bSsToMCZCBl99LQU~In0Xx9mioVMx8oCKuXR7JklbzgfTqDBEDtVOuYBZ-wEU0hcuxO771-zJDHDp9eTKTHI5yt63tmumHD4Rs-zZqVF23COLkU21SGJwYeprJ-gk93ohYbteqaw7l8vGG3Gsed2p-Ffcd8pgvv5aR0TITrNg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1260608"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1260608/Synthesis_of_Polymer_Derived_Boron_Doped_Rare_Earth_Stabilized_Bismuth_Oxide_Nanocomposites_for_SOFC_Applications"><img alt="Research paper thumbnail of Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1260608/Synthesis_of_Polymer_Derived_Boron_Doped_Rare_Earth_Stabilized_Bismuth_Oxide_Nanocomposites_for_SOFC_Applications">Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for S...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications<br /><br />İbrahim USLU<br /><br /><br />Nanoscale composite materials in the form of nanopowders, nanowires, nanofibers and nanorods constitute a rapidly growing field, in terms of both scientific interest and potential technological applications [1-4]. Recently, polymer derived nanocomposites has become increasingly important in for numerous technological applications such as solid oxide fuel cells (SOFCs) [5]. <br /><br />Solid oxide fuel cells (SOFC) are based on the concept of oxygen ion conducting electrolyte through which the oxide ions (O2-) migrate from the air electrode (cathode) side to the fuel electrode (anode) side where they react with the fuel (H2, CH4, etc.) to generate an electrical voltage. [6] One major issue in the development of SOFC is the development of electrolyte materials with sufficiently high ionic conductivity at temperature below 800 °C. Lowering the operation temperatures would lessen the materials constraints and reduce the cost to fabricate the cell. <br /><br />Bismuth oxide (Bi2O3) is an interesting transition metal oxide, with a large energy gap, dielectric permittivity [7,8] with low toxicity and low melting temperature (824 °C), has been identified to be the best ionic-conductive oxide at temperatures higher than 730 °C. Therefore, it is a potential electrolyte for solid oxide fuel cell (SOFC) [9]. However, bismuth oxide tends to be unstable and its conductive characteristics are not retained over longer periods of time, but cubic δ-Bi2O3 phase attracts particular attention. Unfortunately, the δ-Bi2O3 is only stable in a temperature range varying between 730–825 °C. When cooler, the δ-Bi2O3 phase transforms to metastable forms and the conductivity drops over three orders of magnitude [9,10]. When hotter, the δ-Bi2O3 phase can be retained at lower temperatures by doping Bi2O3 with the rare earth<br /><br />The δ-Bi2O3 with 25% of oxygen vacancies also exhibits very high O2- ion conductivity with respect to other phases of Bi2O3 namely α, β and γ phases. A large number of studies has shown that the high conductivity δ-phase in Bi2O3 could be stabilized at lower temperatures, the addition of rare earth dopants (for example, Yb2O3, Er2O3, Dy2O3, Gd2O3) [11]. <br /><br />The addition of boron oxide to the composite materials as a dopant is very beneficial. It is an effective sintering aid because of its low melting point (460 °C), which could help during the sintering process. In this study, boric acid was chosen as the cheapest and nontoxic source of boric oxide [12-14].<br /><br />The polymer precursor technique (PPT) has been proven to be one of the suitable techniques for the preparation of composite oxide which employs of complexing of metal acetate/nitrate precursor in a polymer solution for example PVA. Formation of low cost resultant polymeric product is calcined at a high temperature to remove the polymer and obtain homogeneous and unagglomerated crystalline ceramic powders. The main advantages of polymeric precursor techniques are the homogeneity of the precursors on a molecular level, the low processing temperatures. In this study, boron doped rare earth stabilized bismuth oxide nanocomposites were produced using PPT technique and PVA as a precursor polymeric material. Nanofibers were obtained using electrospinning technique, and then obtained nanofibers were turned into ceramic powders via calcination process. Nanofibers and ceramic powder samples were characterized by FT-IR, XRD and SEM techniques. Crystallite sizes of the samples were evaluated using Scherrer’s equation. Surface area and porosity of the powders was evaluated using BET technique.<br /><br />Composite powders with nanograin size were obtained from this study. Nanograins have greater ratios of surface area to volume, which means a greater ratio of grain boundary to dislocations. The more grain boundaries that exist, the higher the strength becomes. Thus, an easy way to improve the strength of a material is to make the grains as small as possible, increasing the amount of grain boundary<br /><br />References<br /><br />1] A. Gholami, H. Tavanai, A.R. Moradi: J. Nanopart. Res. 13 (2011) 2089.<br />[2] D. Parlevliet, P. Jennings: J. Nanopart. Res. 13 (2011) 4431. <br />[3] K.M. Sawicka, P. Gouma: J. Nanopart. Res. 8 (2006) 769.<br />[4] C.W. Blackledge, T. Tabarin, E. Masson, R.J. Forster, T.E. Keyes: J. Nanopart. Res. 13 (2011) 4659.<br />[5] D.J. Guo, S.K. Cui, H. Sun: J. Nanopart. Res. 11 (2009) 707.<br />[6] S.C. Singhal: Solid State Ionics 135 (2000) 305.<br />[7] L. Leontie, G.I. Rusu: J. Non-Cryst. Solids 352 (2006) 1475.<br />[8] D.F. Peng, H.Q. Sun, X.S. Wang, J.C. Zhang, M.M. Tang, X. Yao: J. Alloy. Compd. 511 (2012) 159. <br />[9] C.H. Weng, W.C.J. Wei: J. Am. Ceram. Soc. 93 (2010) 3124.<br />[10] A.M. Azad, S. Larose, S.A. Akbar: J. Mater. Sci. 29 (1994) 4135.<br />[11] M. Bosacka: Mater. Res. Bull. 41 (2006) 2181.<br />[12] M. Takeyama, C.T. Liu: Acta. Metall. Sin. 36 (1988) 1241.<br />[13] Z.W. Zhang, C.T. Liu, S. Guo, J.L. Cheng, G. Chen, T. Fujita, M.W. Chen, Y.W. Chung, S. Vaynman, M.E. Fine, B.A. Chin: Mat. Sci. Eng. A-Struct. 528 (2011) 855.<br />[14] J.M. Ting: J. Am. Ceram. Soc. 77 (1994) 2751.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="344527026ccefc6e491e683c91ced3c9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:21006238,&quot;asset_id&quot;:1260608,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/21006238/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1260608"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1260608"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1260608; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1260608]").text(description); $(".js-view-count[data-work-id=1260608]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1260608; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1260608']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1260608, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "344527026ccefc6e491e683c91ced3c9" } } $('.js-work-strip[data-work-id=1260608]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1260608,"title":"Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications","translated_title":"","metadata":{"abstract":"Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications\n\nİbrahim USLU\n\n\nNanoscale composite materials in the form of nanopowders, nanowires, nanofibers and nanorods constitute a rapidly growing field, in terms of both scientific interest and potential technological applications [1-4]. Recently, polymer derived nanocomposites has become increasingly important in for numerous technological applications such as solid oxide fuel cells (SOFCs) [5]. \n\nSolid oxide fuel cells (SOFC) are based on the concept of oxygen ion conducting electrolyte through which the oxide ions (O2-) migrate from the air electrode (cathode) side to the fuel electrode (anode) side where they react with the fuel (H2, CH4, etc.) to generate an electrical voltage. [6] One major issue in the development of SOFC is the development of electrolyte materials with sufficiently high ionic conductivity at temperature below 800 °C. Lowering the operation temperatures would lessen the materials constraints and reduce the cost to fabricate the cell. \n\nBismuth oxide (Bi2O3) is an interesting transition metal oxide, with a large energy gap, dielectric permittivity [7,8] with low toxicity and low melting temperature (824 °C), has been identified to be the best ionic-conductive oxide at temperatures higher than 730 °C. Therefore, it is a potential electrolyte for solid oxide fuel cell (SOFC) [9]. However, bismuth oxide tends to be unstable and its conductive characteristics are not retained over longer periods of time, but cubic δ-Bi2O3 phase attracts particular attention. Unfortunately, the δ-Bi2O3 is only stable in a temperature range varying between 730–825 °C. When cooler, the δ-Bi2O3 phase transforms to metastable forms and the conductivity drops over three orders of magnitude [9,10]. When hotter, the δ-Bi2O3 phase can be retained at lower temperatures by doping Bi2O3 with the rare earth\n\nThe δ-Bi2O3 with 25% of oxygen vacancies also exhibits very high O2- ion conductivity with respect to other phases of Bi2O3 namely α, β and γ phases. A large number of studies has shown that the high conductivity δ-phase in Bi2O3 could be stabilized at lower temperatures, the addition of rare earth dopants (for example, Yb2O3, Er2O3, Dy2O3, Gd2O3) [11]. \n\nThe addition of boron oxide to the composite materials as a dopant is very beneficial. It is an effective sintering aid because of its low melting point (460 °C), which could help during the sintering process. In this study, boric acid was chosen as the cheapest and nontoxic source of boric oxide [12-14].\n\nThe polymer precursor technique (PPT) has been proven to be one of the suitable techniques for the preparation of composite oxide which employs of complexing of metal acetate/nitrate precursor in a polymer solution for example PVA. Formation of low cost resultant polymeric product is calcined at a high temperature to remove the polymer and obtain homogeneous and unagglomerated crystalline ceramic powders. The main advantages of polymeric precursor techniques are the homogeneity of the precursors on a molecular level, the low processing temperatures. In this study, boron doped rare earth stabilized bismuth oxide nanocomposites were produced using PPT technique and PVA as a precursor polymeric material. Nanofibers were obtained using electrospinning technique, and then obtained nanofibers were turned into ceramic powders via calcination process. Nanofibers and ceramic powder samples were characterized by FT-IR, XRD and SEM techniques. Crystallite sizes of the samples were evaluated using Scherrer’s equation. Surface area and porosity of the powders was evaluated using BET technique.\n\nComposite powders with nanograin size were obtained from this study. Nanograins have greater ratios of surface area to volume, which means a greater ratio of grain boundary to dislocations. The more grain boundaries that exist, the higher the strength becomes. Thus, an easy way to improve the strength of a material is to make the grains as small as possible, increasing the amount of grain boundary\n\nReferences\n\n1] A. Gholami, H. Tavanai, A.R. Moradi: J. Nanopart. Res. 13 (2011) 2089.\n[2] D. Parlevliet, P. Jennings: J. Nanopart. Res. 13 (2011) 4431. \n[3] K.M. Sawicka, P. Gouma: J. Nanopart. Res. 8 (2006) 769.\n[4] C.W. Blackledge, T. Tabarin, E. Masson, R.J. Forster, T.E. Keyes: J. Nanopart. Res. 13 (2011) 4659.\n[5] D.J. Guo, S.K. Cui, H. Sun: J. Nanopart. Res. 11 (2009) 707.\n[6] S.C. Singhal: Solid State Ionics 135 (2000) 305.\n[7] L. Leontie, G.I. Rusu: J. Non-Cryst. Solids 352 (2006) 1475.\n[8] D.F. Peng, H.Q. Sun, X.S. Wang, J.C. Zhang, M.M. Tang, X. Yao: J. Alloy. Compd. 511 (2012) 159. \n[9] C.H. Weng, W.C.J. Wei: J. Am. Ceram. Soc. 93 (2010) 3124.\n[10] A.M. Azad, S. Larose, S.A. Akbar: J. Mater. Sci. 29 (1994) 4135.\n[11] M. Bosacka: Mater. Res. Bull. 41 (2006) 2181.\n[12] M. Takeyama, C.T. Liu: Acta. Metall. Sin. 36 (1988) 1241.\n[13] Z.W. Zhang, C.T. Liu, S. Guo, J.L. Cheng, G. Chen, T. Fujita, M.W. Chen, Y.W. Chung, S. Vaynman, M.E. Fine, B.A. Chin: Mat. Sci. Eng. A-Struct. 528 (2011) 855.\n[14] J.M. Ting: J. Am. Ceram. Soc. 77 (1994) 2751.\n\n","organization":"Prof.Dr. İbrahim USLU İnvited Speaker 8. Nanoscience and Nanotechnolgy Congress (VIII. Türkiye Nanobilim - Nanoteknoloji Kongresi) Hacettepe University, Ankara, 25-28 July, 2012","conference_end_date":{"day":28,"month":6,"year":2012,"errors":{}},"conference_start_date":{"day":25,"month":6,"year":2012,"errors":{}}},"translated_abstract":"Synthesis of Polymer Derived Boron-Doped Rare Earth Stabilized Bismuth Oxide Nanocomposites for SOFC Applications\n\nİbrahim USLU\n\n\nNanoscale composite materials in the form of nanopowders, nanowires, nanofibers and nanorods constitute a rapidly growing field, in terms of both scientific interest and potential technological applications [1-4]. Recently, polymer derived nanocomposites has become increasingly important in for numerous technological applications such as solid oxide fuel cells (SOFCs) [5]. \n\nSolid oxide fuel cells (SOFC) are based on the concept of oxygen ion conducting electrolyte through which the oxide ions (O2-) migrate from the air electrode (cathode) side to the fuel electrode (anode) side where they react with the fuel (H2, CH4, etc.) to generate an electrical voltage. [6] One major issue in the development of SOFC is the development of electrolyte materials with sufficiently high ionic conductivity at temperature below 800 °C. Lowering the operation temperatures would lessen the materials constraints and reduce the cost to fabricate the cell. \n\nBismuth oxide (Bi2O3) is an interesting transition metal oxide, with a large energy gap, dielectric permittivity [7,8] with low toxicity and low melting temperature (824 °C), has been identified to be the best ionic-conductive oxide at temperatures higher than 730 °C. Therefore, it is a potential electrolyte for solid oxide fuel cell (SOFC) [9]. However, bismuth oxide tends to be unstable and its conductive characteristics are not retained over longer periods of time, but cubic δ-Bi2O3 phase attracts particular attention. Unfortunately, the δ-Bi2O3 is only stable in a temperature range varying between 730–825 °C. When cooler, the δ-Bi2O3 phase transforms to metastable forms and the conductivity drops over three orders of magnitude [9,10]. When hotter, the δ-Bi2O3 phase can be retained at lower temperatures by doping Bi2O3 with the rare earth\n\nThe δ-Bi2O3 with 25% of oxygen vacancies also exhibits very high O2- ion conductivity with respect to other phases of Bi2O3 namely α, β and γ phases. A large number of studies has shown that the high conductivity δ-phase in Bi2O3 could be stabilized at lower temperatures, the addition of rare earth dopants (for example, Yb2O3, Er2O3, Dy2O3, Gd2O3) [11]. \n\nThe addition of boron oxide to the composite materials as a dopant is very beneficial. It is an effective sintering aid because of its low melting point (460 °C), which could help during the sintering process. In this study, boric acid was chosen as the cheapest and nontoxic source of boric oxide [12-14].\n\nThe polymer precursor technique (PPT) has been proven to be one of the suitable techniques for the preparation of composite oxide which employs of complexing of metal acetate/nitrate precursor in a polymer solution for example PVA. Formation of low cost resultant polymeric product is calcined at a high temperature to remove the polymer and obtain homogeneous and unagglomerated crystalline ceramic powders. The main advantages of polymeric precursor techniques are the homogeneity of the precursors on a molecular level, the low processing temperatures. In this study, boron doped rare earth stabilized bismuth oxide nanocomposites were produced using PPT technique and PVA as a precursor polymeric material. Nanofibers were obtained using electrospinning technique, and then obtained nanofibers were turned into ceramic powders via calcination process. Nanofibers and ceramic powder samples were characterized by FT-IR, XRD and SEM techniques. Crystallite sizes of the samples were evaluated using Scherrer’s equation. Surface area and porosity of the powders was evaluated using BET technique.\n\nComposite powders with nanograin size were obtained from this study. Nanograins have greater ratios of surface area to volume, which means a greater ratio of grain boundary to dislocations. The more grain boundaries that exist, the higher the strength becomes. Thus, an easy way to improve the strength of a material is to make the grains as small as possible, increasing the amount of grain boundary\n\nReferences\n\n1] A. Gholami, H. Tavanai, A.R. Moradi: J. Nanopart. Res. 13 (2011) 2089.\n[2] D. Parlevliet, P. Jennings: J. Nanopart. Res. 13 (2011) 4431. \n[3] K.M. Sawicka, P. Gouma: J. Nanopart. Res. 8 (2006) 769.\n[4] C.W. Blackledge, T. Tabarin, E. Masson, R.J. Forster, T.E. Keyes: J. Nanopart. Res. 13 (2011) 4659.\n[5] D.J. Guo, S.K. Cui, H. Sun: J. Nanopart. Res. 11 (2009) 707.\n[6] S.C. Singhal: Solid State Ionics 135 (2000) 305.\n[7] L. Leontie, G.I. Rusu: J. Non-Cryst. Solids 352 (2006) 1475.\n[8] D.F. Peng, H.Q. Sun, X.S. Wang, J.C. Zhang, M.M. Tang, X. Yao: J. Alloy. Compd. 511 (2012) 159. \n[9] C.H. Weng, W.C.J. Wei: J. Am. Ceram. Soc. 93 (2010) 3124.\n[10] A.M. Azad, S. Larose, S.A. Akbar: J. Mater. Sci. 29 (1994) 4135.\n[11] M. Bosacka: Mater. Res. Bull. 41 (2006) 2181.\n[12] M. Takeyama, C.T. Liu: Acta. Metall. Sin. 36 (1988) 1241.\n[13] Z.W. Zhang, C.T. Liu, S. Guo, J.L. Cheng, G. Chen, T. Fujita, M.W. Chen, Y.W. Chung, S. Vaynman, M.E. Fine, B.A. Chin: Mat. Sci. Eng. A-Struct. 528 (2011) 855.\n[14] J.M. Ting: J. Am. Ceram. Soc. 77 (1994) 2751.\n\n","internal_url":"https://www.academia.edu/1260608/Synthesis_of_Polymer_Derived_Boron_Doped_Rare_Earth_Stabilized_Bismuth_Oxide_Nanocomposites_for_SOFC_Applications","translated_internal_url":"","created_at":"2012-06-26T20:52:19.734-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":21006238,"title":"","file_type":"ppsx","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"SOFC.ppsx","download_url":"https://www.academia.edu/attachments/21006238/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_of_Polymer_Derived_Boron_Doped.ppsx","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/21006238/SOFC.ppsx?1340769202=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_of_Polymer_Derived_Boron_Doped.ppsx\u0026Expires=1731454491\u0026Signature=ZaL20s7lX5suLNLSUqjPpeIIYBjNEA48zBjJwrjPnQpxS4mbyAk84k2HRtRzY-8ce5t9NOKbR~sbTcaqDaarZpEMXp2DZ~x61IU07owx5Ovs5TQVBvUMm-O0Qm3IdThEfSF4Erph6Gw7Sty4jMtngNxf7DGpnpBYoAHxxzE9Ys9kSvZSZgIgnUg6ssVeCoMgY3WQXeXhi-GtTz870dK4w4DV82~vO9Iipqp1992UZHT5zAPkknUpKsPIB8N8zUVxvw-NfRBi0DpICHZ9OlczC7eV9aLbBvN3n0LtoygPKQWp2KHFOT6y21dqrufP3MZcZO2OJKr9FqeIbr4rGzVRCg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Synthesis_of_Polymer_Derived_Boron_Doped_Rare_Earth_Stabilized_Bismuth_Oxide_Nanocomposites_for_SOFC_Applications","translated_slug":"","page_count":69,"language":"en","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":21006238,"title":"","file_type":"ppsx","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"SOFC.ppsx","download_url":"https://www.academia.edu/attachments/21006238/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_of_Polymer_Derived_Boron_Doped.ppsx","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/21006238/SOFC.ppsx?1340769202=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_of_Polymer_Derived_Boron_Doped.ppsx\u0026Expires=1731454491\u0026Signature=ZaL20s7lX5suLNLSUqjPpeIIYBjNEA48zBjJwrjPnQpxS4mbyAk84k2HRtRzY-8ce5t9NOKbR~sbTcaqDaarZpEMXp2DZ~x61IU07owx5Ovs5TQVBvUMm-O0Qm3IdThEfSF4Erph6Gw7Sty4jMtngNxf7DGpnpBYoAHxxzE9Ys9kSvZSZgIgnUg6ssVeCoMgY3WQXeXhi-GtTz870dK4w4DV82~vO9Iipqp1992UZHT5zAPkknUpKsPIB8N8zUVxvw-NfRBi0DpICHZ9OlczC7eV9aLbBvN3n0LtoygPKQWp2KHFOT6y21dqrufP3MZcZO2OJKr9FqeIbr4rGzVRCg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1258546"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1258546/Fabrication_and_thermoelectric_properties_of_NaCo2O4_PVA_polymerized_complex"><img alt="Research paper thumbnail of Fabrication and thermoelectric properties of NaCo2O4 PVA polymerized complex" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1258546/Fabrication_and_thermoelectric_properties_of_NaCo2O4_PVA_polymerized_complex">Fabrication and thermoelectric properties of NaCo2O4 PVA polymerized complex</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Sodium cobalt oxide (Na1Co2O4) crystalline thermoelectric materials were obtained using polyvinyl...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Sodium cobalt oxide (Na1Co2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD), scaning electron microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The sol-gel solution calcined at 800 oC and then calcined powder was pellet 12,5 t under pressure and sintered at the&nbsp; 850 oC.&nbsp; This pellets thermoelectric properties measured by Lot-Oriel PPMS.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="382fc4c2f1d391cc5fa1971f52f3d86f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:20854647,&quot;asset_id&quot;:1258546,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/20854647/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1258546"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1258546"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1258546; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1258546]").text(description); $(".js-view-count[data-work-id=1258546]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1258546; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1258546']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1258546, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "382fc4c2f1d391cc5fa1971f52f3d86f" } } $('.js-work-strip[data-work-id=1258546]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1258546,"title":"Fabrication and thermoelectric properties of NaCo2O4 PVA polymerized complex","translated_title":"","metadata":{"abstract":"Sodium cobalt oxide (Na1Co2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD), scaning electron microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The sol-gel solution calcined at 800 oC and then calcined powder was pellet 12,5 t under pressure and sintered at the 850 oC. This pellets thermoelectric properties measured by Lot-Oriel PPMS.","more_info":"Mehmet Okan Erdal, Mustafa Koyuncu, İbrahim Uslu, Haziret Durmuş","event_date":{"day":25,"month":6,"year":2012,"errors":{}},"conference_end_date":{"day":28,"month":6,"year":2012,"errors":{}},"conference_start_date":{"day":25,"month":6,"year":2012,"errors":{}}},"translated_abstract":"Sodium cobalt oxide (Na1Co2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD), scaning electron microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The sol-gel solution calcined at 800 oC and then calcined powder was pellet 12,5 t under pressure and sintered at the 850 oC. This pellets thermoelectric properties measured by Lot-Oriel PPMS.","internal_url":"https://www.academia.edu/1258546/Fabrication_and_thermoelectric_properties_of_NaCo2O4_PVA_polymerized_complex","translated_internal_url":"","created_at":"2012-06-26T01:52:09.593-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":20854647,"title":"","file_type":"ppt","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"Poster-yeni.ppt","download_url":"https://www.academia.edu/attachments/20854647/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Fabrication_and_thermoelectric_propertie.ppt","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/20854647/Poster-yeni.ppt?1340700325=\u0026response-content-disposition=attachment%3B+filename%3DFabrication_and_thermoelectric_propertie.ppt\u0026Expires=1733756524\u0026Signature=PYYVl~~9sQdUczqyduK8YbGJUQoiSziCm2G3nFsg1tXcAE2JiQxoTZSn4YmrabIghd7aBmkWwHcUezaxjedHxglgd-qFW9XFdyFjD6pjzyTBEt2KYRNm0pAfgyHGQhdQ3t2x22~4zSwz84NZueeCp8HuZ-JkZk8m8RAygcjsq2SAbhpykcLez3UEeCku0HxterRX~DXEUd~42xvCCPtEb9jfO~W6kwSjF3C0B0YRA1ahzYWL0W-q8Qcj-7Vc~fpcke4B7LWDRY4KIjVy0Vfllc8LqTIkWOOlGfDJN2Cn3PP1nl1Yp~NxhNVGmXNfsA37IT7Zz~r9U8xr0xcLUP88sQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Fabrication_and_thermoelectric_properties_of_NaCo2O4_PVA_polymerized_complex","translated_slug":"","page_count":1,"language":"en","content_type":"Work","summary":"Sodium cobalt oxide (Na1Co2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD), scaning electron microscopy (SEM) and Fourier transform infrared spectroscopy (FTIR). The sol-gel solution calcined at 800 oC and then calcined powder was pellet 12,5 t under pressure and sintered at the 850 oC. This pellets thermoelectric properties measured by Lot-Oriel PPMS.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":20854647,"title":"","file_type":"ppt","scribd_thumbnail_url":"https://a.academia-assets.com/images/blank-paper.jpg","file_name":"Poster-yeni.ppt","download_url":"https://www.academia.edu/attachments/20854647/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Fabrication_and_thermoelectric_propertie.ppt","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/20854647/Poster-yeni.ppt?1340700325=\u0026response-content-disposition=attachment%3B+filename%3DFabrication_and_thermoelectric_propertie.ppt\u0026Expires=1733756524\u0026Signature=PYYVl~~9sQdUczqyduK8YbGJUQoiSziCm2G3nFsg1tXcAE2JiQxoTZSn4YmrabIghd7aBmkWwHcUezaxjedHxglgd-qFW9XFdyFjD6pjzyTBEt2KYRNm0pAfgyHGQhdQ3t2x22~4zSwz84NZueeCp8HuZ-JkZk8m8RAygcjsq2SAbhpykcLez3UEeCku0HxterRX~DXEUd~42xvCCPtEb9jfO~W6kwSjF3C0B0YRA1ahzYWL0W-q8Qcj-7Vc~fpcke4B7LWDRY4KIjVy0Vfllc8LqTIkWOOlGfDJN2Cn3PP1nl1Yp~NxhNVGmXNfsA37IT7Zz~r9U8xr0xcLUP88sQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1709953"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1709953/Preparation_of_Nanoceramic_La_Doped_Bi2O3"><img alt="Research paper thumbnail of Preparation of Nanoceramic La-Doped Bi2O3" class="work-thumbnail" src="https://attachments.academia-assets.com/7501426/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1709953/Preparation_of_Nanoceramic_La_Doped_Bi2O3">Preparation of Nanoceramic La-Doped Bi2O3</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Electrospinning process was utilized to fabricate lantanium doped bismuth ultrafine nanofibers. P...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Electrospinning process was utilized to fabricate lantanium doped bismuth ultrafine nanofibers. PVA was used as polymer solution with bismuth acetate/lantanium acetate, followed by calcination at 800 oC. The produced nanofibers and calcined crystal structures were characterized by using scanning electron microscopy (SEM) and X-ray diffraction (XRD). The results indicated that samples after calcination should be sintered more than one to obtain pure crystalline phase.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="41c49778a012874fb94de7fc90f91fb7" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7501426,&quot;asset_id&quot;:1709953,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7501426/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709953"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709953"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709953; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709953]").text(description); $(".js-view-count[data-work-id=1709953]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709953; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709953']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709953, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "41c49778a012874fb94de7fc90f91fb7" } } $('.js-work-strip[data-work-id=1709953]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709953,"title":"Preparation of Nanoceramic La-Doped Bi2O3","translated_title":"","metadata":{"abstract":"Electrospinning process was utilized to fabricate lantanium doped bismuth ultrafine nanofibers. PVA was used as polymer solution with bismuth acetate/lantanium acetate, followed by calcination at 800 oC. The produced nanofibers and calcined crystal structures were characterized by using scanning electron microscopy (SEM) and X-ray diffraction (XRD). The results indicated that samples after calcination should be sintered more than one to obtain pure crystalline phase.","location":"The 6th Nanoscience and Nanotechnology Conference (NanoTR6) will be held in Golden Dolphin Hotel, Izmir Cesme","more_info":"Ş. Durmuşoğlu, A. Aytimur, S. Keskin, Ibrahim Uslu, A. Akdemir","conference_end_date":{"day":18,"month":6,"year":2010,"errors":{}},"conference_start_date":{"day":15,"month":6,"year":2010,"errors":{}}},"translated_abstract":"Electrospinning process was utilized to fabricate lantanium doped bismuth ultrafine nanofibers. PVA was used as polymer solution with bismuth acetate/lantanium acetate, followed by calcination at 800 oC. The produced nanofibers and calcined crystal structures were characterized by using scanning electron microscopy (SEM) and X-ray diffraction (XRD). The results indicated that samples after calcination should be sintered more than one to obtain pure crystalline phase.","internal_url":"https://www.academia.edu/1709953/Preparation_of_Nanoceramic_La_Doped_Bi2O3","translated_internal_url":"","created_at":"2012-01-07T22:54:19.656-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7501426,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7501426/thumbnails/1.jpg","file_name":"preparation.pdf","download_url":"https://www.academia.edu/attachments/7501426/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Preparation_of_Nanoceramic_La_Doped_Bi2O.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7501426/preparation-libre.pdf?1390851657=\u0026response-content-disposition=attachment%3B+filename%3DPreparation_of_Nanoceramic_La_Doped_Bi2O.pdf\u0026Expires=1733756524\u0026Signature=ZoCrN3tgQ3OtJYyeDcvS9SFOVCB79ZFaIKuIN56CPDsYCW70W2NM0AkmEnJRqj941d4DmCjKpiYdSWFU9dNNI9gyemfcJCsHJAZZzxBDsME5NVGxzy~SwLZO-iUqcmTpEgwe1vZATYfHjC0N15zh6QT6DSFRpbISmKbvNlYLnWxf5VKmrF32prHhoqgAMhEcp0crl2pmUKkSDxu0ciG8-LDSQJCxZeKhuT6Tr6rv-IeUq9AE12PbF~Vq1nJC~RGcHEXfE2t0BghKmzRGAEjUNVArbzVws4g9upVMPnpfDSVbsebjB2tx~MP-NDVnfmiIsIMU3U6hNedwE7~VJx5Cgg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Preparation_of_Nanoceramic_La_Doped_Bi2O3","translated_slug":"","page_count":1,"language":"en","content_type":"Work","summary":"Electrospinning process was utilized to fabricate lantanium doped bismuth ultrafine nanofibers. PVA was used as polymer solution with bismuth acetate/lantanium acetate, followed by calcination at 800 oC. The produced nanofibers and calcined crystal structures were characterized by using scanning electron microscopy (SEM) and X-ray diffraction (XRD). 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PVA was used as polymer solution with sodium acetate/cobalt acetate, followed by calcination at 800 oC. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD). The sol-gel solution calcined at 800 oC and then sintered at the same temperature was single crystal and XRD results have an agreement with the literature values. The results indicated that the polymeric sol-gel method is a promising process for the synthesis of sodium cobalt oxide thermoelectric materials.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1142e46b803530b6df4a6fd05bf4400f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7501622,&quot;asset_id&quot;:1709954,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7501622/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709954"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709954"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709954; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709954]").text(description); $(".js-view-count[data-work-id=1709954]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709954; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709954']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709954, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "1142e46b803530b6df4a6fd05bf4400f" } } $('.js-work-strip[data-work-id=1709954]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709954,"title":"Synthesis and Characterization of NaxCo2O4 Thermoelectric Material Using PVA Polymerized Complex","translated_title":"","metadata":{"abstract":"For the first time, sodium cobalt oxide (NaxCo2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate, followed by calcination at 800 oC. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD). The sol-gel solution calcined at 800 oC and then sintered at the same temperature was single crystal and XRD results have an agreement with the literature values. The results indicated that the polymeric sol-gel method is a promising process for the synthesis of sodium cobalt oxide thermoelectric materials.","location":"The 6th Nanoscience and Nanotechnology Conference (NanoTR6) will be held in Golden Dolphin Hotel, Izmir Cesme,","more_info":"Mehmet Okan Erdal1, İbrahim Uslu, Arda Aytimur , Mustafa Koyuncu","conference_end_date":{"day":18,"month":6,"year":2010,"errors":{}},"conference_start_date":{"day":15,"month":6,"year":2010,"errors":{}}},"translated_abstract":"For the first time, sodium cobalt oxide (NaxCo2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate, followed by calcination at 800 oC. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD). The sol-gel solution calcined at 800 oC and then sintered at the same temperature was single crystal and XRD results have an agreement with the literature values. The results indicated that the polymeric sol-gel method is a promising process for the synthesis of sodium cobalt oxide thermoelectric materials.","internal_url":"https://www.academia.edu/1709954/Synthesis_and_Characterization_of_NaxCo2O4_Thermoelectric_Material_Using_PVA_Polymerized_Complex","translated_internal_url":"","created_at":"2012-01-07T23:16:40.524-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7501622,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7501622/thumbnails/1.jpg","file_name":"synthesis.pdf","download_url":"https://www.academia.edu/attachments/7501622/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_and_Characterization_of_NaxCo2.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7501622/synthesis-libre.pdf?1390851661=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_and_Characterization_of_NaxCo2.pdf\u0026Expires=1733756524\u0026Signature=ONmdoBYruWSgZvCJmbSTDbNDypQUIqIqQrSuTY1HuG~9njuDRRM52FUk5mPM4uv6VhOeBeZ434OPOzvwMufePgHRvPmismxk4W1EjRpLruCkIBDrUzbn~cQvWCi16-GuAanuNqCRVIfiEUtLcuPzRwwsiM-naq5WUC7lTf9A5R43K7mJthLPLa9th3yu3UstKLPgEsrvcGWreaTlGr2GMlYbml-J3o4MMc2iN-MlNyZ2mBoGl9~sEDMeBO8XhnMldNPHOoaOB8pfNzZTBwndo9ZPybMdI8yLZpZ6kGqYH22cdvADEf~mEU-LTcTCbQBtPQsl4W9WdkfH1qbgPo2KGw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Synthesis_and_Characterization_of_NaxCo2O4_Thermoelectric_Material_Using_PVA_Polymerized_Complex","translated_slug":"","page_count":1,"language":"en","content_type":"Work","summary":"For the first time, sodium cobalt oxide (NaxCo2O4) crystalline thermoelectric materials were obtained using polyvinyl alcohol (PVA) polymerized complex sol-gel solution. PVA was used as polymer solution with sodium acetate/cobalt acetate, followed by calcination at 800 oC. The sodium cobalt oxide calcined crystal structures were characterized by X-ray diffraction (XRD). The sol-gel solution calcined at 800 oC and then sintered at the same temperature was single crystal and XRD results have an agreement with the literature values. The results indicated that the polymeric sol-gel method is a promising process for the synthesis of sodium cobalt oxide thermoelectric materials.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7501622,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7501622/thumbnails/1.jpg","file_name":"synthesis.pdf","download_url":"https://www.academia.edu/attachments/7501622/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_and_Characterization_of_NaxCo2.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7501622/synthesis-libre.pdf?1390851661=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_and_Characterization_of_NaxCo2.pdf\u0026Expires=1733756525\u0026Signature=JFZREQmqy2O8jtXbcixGxyxJ1m~FWfH3wM-53liocp9BIfVMwGVxnI-agnaueLp9mrB4RvuB0h4kC5CE3To-YfhEcghJYwqLYUiw3M~TY9hRk56vCBaT4uDLsiFMvfk1fg7rrq5ITCg1lgHmDRgraHrY38qgzdiMgbIqvSXHqXxqDl2kV6uIMcF~BD7QwHg3vfMXqeoi4vJEwjXWrAMmR0Uuz6bku8c5ShRsWSeKkmwcCRazRonpPfTwS1wUTg-NZIDbEYNEAOQjA8q39mhguH1Kbw1PkmZ8k~tiKXLmgEbhGLtgNeI16d2bJ6uxzaNoq8Iy0-C2Uic1bkK4J80cIg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); 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Bu nedenle ülkemizde nükleer enerji alternatif bir enerji kaynağı olarak devreye girmelidir. Ancak kurulacak reaktörün güvenli işletilmesi gereklidir. Tesisin güvenli işletilmesinde siyasi otoriteden bağımsız Nükleer Düzenleme ve Denetleme Kurumu (NDDK) kurulması son derece önemli ve Uluslar arası Atom Enerjisi Ajansı’nın (IAEA) güvenlik kriterlerine göre de gereklidir. Tesisin kullanacağı nükleer yakıt konusunda dışa bağımlılığı ortadan kaldıracak her türlü çalışma ve ARGE çalışmaları başta üniversitelerimiz olmak üzere başlatılmalı ve teşvik edilmelidir. 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Bu nedenle ülkemizde nükleer enerji alternatif bir enerji kaynağı olarak devreye girmelidir. Ancak kurulacak reaktörün güvenli işletilmesi gereklidir. Tesisin güvenli işletilmesinde siyasi otoriteden bağımsız Nükleer Düzenleme ve Denetleme Kurumu (NDDK) kurulması son derece önemli ve Uluslar arası Atom Enerjisi Ajansı’nın (IAEA) güvenlik kriterlerine göre de gereklidir. Tesisin kullanacağı nükleer yakıt konusunda dışa bağımlılığı ortadan kaldıracak her türlü çalışma ve ARGE çalışmaları başta üniversitelerimiz olmak üzere başlatılmalı ve teşvik edilmelidir. Kullanılmış nükleer yakıtların derin bir şekilde depolanması ya da işletilmesi konusu da şimdiden ele alınması gerektiren konuların başında gelmektedir.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7502583,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7502583/thumbnails/1.jpg","file_name":"nukleer.pdf","download_url":"https://www.academia.edu/attachments/7502583/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Nukleer_Reaktorlerin_Tipleri_Yakit_Cevri.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7502583/nukleer-libre.pdf?1390851661=\u0026response-content-disposition=attachment%3B+filename%3DNukleer_Reaktorlerin_Tipleri_Yakit_Cevri.pdf\u0026Expires=1733898196\u0026Signature=Z3MRpTNPWUmJ-FYij9q8mNeOduAxrwredLn8dit03Sg5x4vr1QyysK5S8QFiVFyoHCYY7ui3p4JA3W8-oOJybfHD2zmwllaLbnyrcrhQA~~LwRU7O~0P-SNMGwlPdbHbi1UYyub5wlJ3jP0v6dBNYXDE83yLRxwKQvelHWCVvVyx6AflQE7Cs9zw8Ara~0QprXGAqj0qIHxIWJHG~7FWtKCHy71Nf25X94~11PoQvxKrFG7Y--35BT0FQ-C9gszNETl0EygKEBesp0jajk7SXADthdYPrUmEdJqhP~HL3rY0VqabzqsfQnQFf~t6hD3TPoweNIO0puFAcWkUDAHoIQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1709977"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1709977/Bor_katk%C4%B1l%C4%B1_Ni_Zn_Asetat_Kompozit_Nanofiberlar%C4%B1n_Eldesi"><img alt="Research paper thumbnail of Bor katkılı Ni-Zn Asetat Kompozit Nanofiberların Eldesi" class="work-thumbnail" src="https://attachments.academia-assets.com/7504233/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1709977/Bor_katk%C4%B1l%C4%B1_Ni_Zn_Asetat_Kompozit_Nanofiberlar%C4%B1n_Eldesi">Bor katkılı Ni-Zn Asetat Kompozit Nanofiberların Eldesi</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Nikel ve çinko oksit ince film seramik kompozitler elektronik ve kimya endüstrisinde yaygın olara...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Nikel ve çinko oksit ince film seramik kompozitler elektronik ve kimya endüstrisinde yaygın olarak kullanılmaktadır[1-5]. Nikel ve çinko oksit yapıların birlikte kullanıldığı da görülmektedir. Son yıllarda bu oksitler gaz duyarlı, yarı iletken ve yumusak ferrit malzemelerin eldesinde de kullanıldıgı görülmektedir [4-7]. Literatürde bu mallezemelerin birlikte üretiminde fiziksel ve kimyasal buhar çöktürme yöntemleri ,sol-gel yöntemi ve son yıllarda da elektrospinleme kullanıldıgı da görülmektedir[3]. <br />Bu çalışmada nikel ve çinko asetat çözeltileri sulu ortamda çözdürülerek elektrospinleme ile nanofiber elde etmek için tasıyıcı olarak kullanılan polivinil alkol ile birlikta çözdürülmustur. Yukardaki çözeltilere degişik miktarlarda bor katkılayarak borun yarı iletken malzemelerin iletkenliğine, akışkanlığına , yapısına , termal dayanıklılığına etkisi viskosimetre ve kondaktometre, FTIR, SEM, DSC cihazları ile incelenmiştir. <br />Asetat çözeltilerinin akışkanlık ve iletkenlik parametrelerinde parallelik gözlenmiş olup bor katkısının çözeltinin akıskanlıgını arttırdığı iletkenliği ise azalttıgı gözlenmiştir. Dsc analizinde bor katkısının erime noktası yukselmesine ve maddelerin daha yüksek sıcaklıklarda parcalanmasına neden olmustur. Aynı zamanda FTIR ve SEM analizleri ile de maddenin karakterizasyonu<br />Literatürde ilk defa yapılan bu çalısmayla daha üstün özellikli Ni-Zn yarıiletken malzemelerin eldesi gerçeklestirilmiştir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9b468f519a404fd66b3fb8a7bb2c15b2" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7504233,&quot;asset_id&quot;:1709977,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7504233/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709977"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709977"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709977; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709977]").text(description); $(".js-view-count[data-work-id=1709977]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709977; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709977']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709977, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "9b468f519a404fd66b3fb8a7bb2c15b2" } } $('.js-work-strip[data-work-id=1709977]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709977,"title":"Bor katkılı Ni-Zn Asetat Kompozit Nanofiberların Eldesi","translated_title":"","metadata":{"abstract":"Nikel ve çinko oksit ince film seramik kompozitler elektronik ve kimya endüstrisinde yaygın olarak kullanılmaktadır[1-5]. Nikel ve çinko oksit yapıların birlikte kullanıldığı da görülmektedir. Son yıllarda bu oksitler gaz duyarlı, yarı iletken ve yumusak ferrit malzemelerin eldesinde de kullanıldıgı görülmektedir [4-7]. Literatürde bu mallezemelerin birlikte üretiminde fiziksel ve kimyasal buhar çöktürme yöntemleri ,sol-gel yöntemi ve son yıllarda da elektrospinleme kullanıldıgı da görülmektedir[3]. \nBu çalışmada nikel ve çinko asetat çözeltileri sulu ortamda çözdürülerek elektrospinleme ile nanofiber elde etmek için tasıyıcı olarak kullanılan polivinil alkol ile birlikta çözdürülmustur. Yukardaki çözeltilere degişik miktarlarda bor katkılayarak borun yarı iletken malzemelerin iletkenliğine, akışkanlığına , yapısına , termal dayanıklılığına etkisi viskosimetre ve kondaktometre, FTIR, SEM, DSC cihazları ile incelenmiştir. \nAsetat çözeltilerinin akışkanlık ve iletkenlik parametrelerinde parallelik gözlenmiş olup bor katkısının çözeltinin akıskanlıgını arttırdığı iletkenliği ise azalttıgı gözlenmiştir. Dsc analizinde bor katkısının erime noktası yukselmesine ve maddelerin daha yüksek sıcaklıklarda parcalanmasına neden olmustur. Aynı zamanda FTIR ve SEM analizleri ile de maddenin karakterizasyonu\nLiteratürde ilk defa yapılan bu çalısmayla daha üstün özellikli Ni-Zn yarıiletken malzemelerin eldesi gerçeklestirilmiştir.","location":"II. Ulusal Bor Çalıştayı","more_info":"İ. Uslu, A. Yaylı, O. Atakol, M.L. Aksu","organization":"BOREN ve ETİ MADEN sponsorluğunda MTA Ankara'da yapılmıştır.","conference_end_date":{"day":18,"month":4,"year":2008,"errors":{}},"conference_start_date":{"day":17,"month":4,"year":2008,"errors":{}}},"translated_abstract":"Nikel ve çinko oksit ince film seramik kompozitler elektronik ve kimya endüstrisinde yaygın olarak kullanılmaktadır[1-5]. Nikel ve çinko oksit yapıların birlikte kullanıldığı da görülmektedir. Son yıllarda bu oksitler gaz duyarlı, yarı iletken ve yumusak ferrit malzemelerin eldesinde de kullanıldıgı görülmektedir [4-7]. Literatürde bu mallezemelerin birlikte üretiminde fiziksel ve kimyasal buhar çöktürme yöntemleri ,sol-gel yöntemi ve son yıllarda da elektrospinleme kullanıldıgı da görülmektedir[3]. \nBu çalışmada nikel ve çinko asetat çözeltileri sulu ortamda çözdürülerek elektrospinleme ile nanofiber elde etmek için tasıyıcı olarak kullanılan polivinil alkol ile birlikta çözdürülmustur. Yukardaki çözeltilere degişik miktarlarda bor katkılayarak borun yarı iletken malzemelerin iletkenliğine, akışkanlığına , yapısına , termal dayanıklılığına etkisi viskosimetre ve kondaktometre, FTIR, SEM, DSC cihazları ile incelenmiştir. \nAsetat çözeltilerinin akışkanlık ve iletkenlik parametrelerinde parallelik gözlenmiş olup bor katkısının çözeltinin akıskanlıgını arttırdığı iletkenliği ise azalttıgı gözlenmiştir. Dsc analizinde bor katkısının erime noktası yukselmesine ve maddelerin daha yüksek sıcaklıklarda parcalanmasına neden olmustur. Aynı zamanda FTIR ve SEM analizleri ile de maddenin karakterizasyonu\nLiteratürde ilk defa yapılan bu çalısmayla daha üstün özellikli Ni-Zn yarıiletken malzemelerin eldesi gerçeklestirilmiştir.","internal_url":"https://www.academia.edu/1709977/Bor_katk%C4%B1l%C4%B1_Ni_Zn_Asetat_Kompozit_Nanofiberlar%C4%B1n_Eldesi","translated_internal_url":"","created_at":"2012-01-08T02:56:07.610-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7504233,"title":"","file_type":"doc","scribd_thumbnail_url":"https://attachments.academia-assets.com/7504233/thumbnails/1.jpg","file_name":"Ni_zi makale bor.doc","download_url":"https://www.academia.edu/attachments/7504233/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Bor_katkili_Ni_Zn_Asetat_Kompozit_Nanofi.doc","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7504233/Ni_zi%20makale%20bor.doc?1326020156=\u0026response-content-disposition=attachment%3B+filename%3DBor_katkili_Ni_Zn_Asetat_Kompozit_Nanofi.doc\u0026Expires=1733898196\u0026Signature=HEKZ-L1c7dK4Mbbu044xxWszhevCUF9aYXNuKy7DOeiOr911Al39b3OFoiJA6HgQtTnUfyasW1dWJ9Yi7qZ0RHCt~DlYdEfgikTI9RsgDJwrsrEzsvlEXi8u0eX8-ksCT5SuHYGAA7Y7hgA52SLnwIyC9J26uRwbKB1hZEBn48c40ORJYD7PZT1Smq92EcqB27pwpSbGgspd4bERyhxuyYvOVtAmcJfDWOMa4W16zR2-E4asgmwza5l4fedirDRZUIjwFoDxdgGXzGNl1-L-5mbRxtWiOqLBUGCEnRnnBIRSPHHdEN3kDxfHvGSZoR3AT35RPwM~sqD6DEOYVmu3Vw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Bor_katkılı_Ni_Zn_Asetat_Kompozit_Nanofiberların_Eldesi","translated_slug":"","page_count":4,"language":"en","content_type":"Work","summary":"Nikel ve çinko oksit ince film seramik kompozitler elektronik ve kimya endüstrisinde yaygın olarak kullanılmaktadır[1-5]. Nikel ve çinko oksit yapıların birlikte kullanıldığı da görülmektedir. Son yıllarda bu oksitler gaz duyarlı, yarı iletken ve yumusak ferrit malzemelerin eldesinde de kullanıldıgı görülmektedir [4-7]. Literatürde bu mallezemelerin birlikte üretiminde fiziksel ve kimyasal buhar çöktürme yöntemleri ,sol-gel yöntemi ve son yıllarda da elektrospinleme kullanıldıgı da görülmektedir[3]. \nBu çalışmada nikel ve çinko asetat çözeltileri sulu ortamda çözdürülerek elektrospinleme ile nanofiber elde etmek için tasıyıcı olarak kullanılan polivinil alkol ile birlikta çözdürülmustur. Yukardaki çözeltilere degişik miktarlarda bor katkılayarak borun yarı iletken malzemelerin iletkenliğine, akışkanlığına , yapısına , termal dayanıklılığına etkisi viskosimetre ve kondaktometre, FTIR, SEM, DSC cihazları ile incelenmiştir. \nAsetat çözeltilerinin akışkanlık ve iletkenlik parametrelerinde parallelik gözlenmiş olup bor katkısının çözeltinin akıskanlıgını arttırdığı iletkenliği ise azalttıgı gözlenmiştir. Dsc analizinde bor katkısının erime noktası yukselmesine ve maddelerin daha yüksek sıcaklıklarda parcalanmasına neden olmustur. 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In this study, we have prepared calixarene based nano fibers by using several p-sulfonated calixarenes via electro-spinning and examined their structures with some characterization methods such as FTIR, SEM.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="cd41552cc702c3a710bc126e002a12b4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7502283,&quot;asset_id&quot;:1709959,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7502283/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709959"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709959"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709959; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709959]").text(description); $(".js-view-count[data-work-id=1709959]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709959; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709959']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709959, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "cd41552cc702c3a710bc126e002a12b4" } } $('.js-work-strip[data-work-id=1709959]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709959,"title":"Formation and Characterization of PVA/Calix[4]arene Nanofibers","translated_title":"","metadata":{"abstract":"For the first time, nanofibers of PVA/Calix[4]arene nanofibers were prepared by using sol–gel processing and electrospinning technique. 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The first step was the preparation of composite by mixing yttrium, barium and copper acetates with polyvinyl alcohol (PVA) at a suitable temperature. The resulting composite polymer was then electrospun giving nano fibers and finally the resulting nano fibers were subjected to a thermal treatment to obtain superconducting material. The conductivity of the nano fibers obtained was measured with four probe technique. Scanning Electron Microscopy (SEM) were used for the characterization of the nanofibers.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="13600485a656f962b2dab72a8160a62d" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7502449,&quot;asset_id&quot;:1709960,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7502449/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709960"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709960"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709960; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709960]").text(description); $(".js-view-count[data-work-id=1709960]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709960; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709960']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709960, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "13600485a656f962b2dab72a8160a62d" } } $('.js-work-strip[data-work-id=1709960]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709960,"title":"Synthesis and Characterization of Superconducting Nanofibers","translated_title":"","metadata":{"abstract":"This study is related to the preparation of boron supported YBa2Cu3O7 (YBCO) superconducting material. 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Scanning Electron Microscopy (SEM) were used for the characterization of the nanofibers.","internal_url":"https://www.academia.edu/1709960/Synthesis_and_Characterization_of_Superconducting_Nanofibers","translated_internal_url":"","created_at":"2012-01-08T00:31:50.912-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7502449,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7502449/thumbnails/1.jpg","file_name":"super.pdf","download_url":"https://www.academia.edu/attachments/7502449/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_and_Characterization_of_Superc.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7502449/super-libre.pdf?1390851662=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_and_Characterization_of_Superc.pdf\u0026Expires=1733756525\u0026Signature=WZXrlFltyXAWmNzl76fu3SPO6zpBjmboCYZsXgl8uVn4zNq6xSpph-DqzKXp3SCLKqooxr4R367EDrHC6R3~WS0YOaANGlEd9rbaBsWg6u-Ygdtkmu~CH5xQdgwDmWcQSEamw0TVHxrZNXUFpaCTHhnc4NbYSapUJFvaei8ZW7YzLP6pzjBUc71rtlf~KSW2LTemtfd0p1tAn0crdHVtxjzOxSgIkHQYL7JAkFbNEc3GiSJ0QY6qwXd7vYNtwZ9LztOKGq1jm53Ar2bTboPY5vsP4iQf1lzEHUD5XiHhhrH6oM2T7L6CCXncE-jksWZ7h~PXgRiy3p4AZsJ075h8pg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Synthesis_and_Characterization_of_Superconducting_Nanofibers","translated_slug":"","page_count":1,"language":"en","content_type":"Work","summary":"This study is related to the preparation of boron supported YBa2Cu3O7 (YBCO) superconducting material. The first step was the preparation of composite by mixing yttrium, barium and copper acetates with polyvinyl alcohol (PVA) at a suitable temperature. The resulting composite polymer was then electrospun giving nano fibers and finally the resulting nano fibers were subjected to a thermal treatment to obtain superconducting material. The conductivity of the nano fibers obtained was measured with four probe technique. Scanning Electron Microscopy (SEM) were used for the characterization of the nanofibers.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7502449,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7502449/thumbnails/1.jpg","file_name":"super.pdf","download_url":"https://www.academia.edu/attachments/7502449/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Synthesis_and_Characterization_of_Superc.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7502449/super-libre.pdf?1390851662=\u0026response-content-disposition=attachment%3B+filename%3DSynthesis_and_Characterization_of_Superc.pdf\u0026Expires=1733756525\u0026Signature=WZXrlFltyXAWmNzl76fu3SPO6zpBjmboCYZsXgl8uVn4zNq6xSpph-DqzKXp3SCLKqooxr4R367EDrHC6R3~WS0YOaANGlEd9rbaBsWg6u-Ygdtkmu~CH5xQdgwDmWcQSEamw0TVHxrZNXUFpaCTHhnc4NbYSapUJFvaei8ZW7YzLP6pzjBUc71rtlf~KSW2LTemtfd0p1tAn0crdHVtxjzOxSgIkHQYL7JAkFbNEc3GiSJ0QY6qwXd7vYNtwZ9LztOKGq1jm53Ar2bTboPY5vsP4iQf1lzEHUD5XiHhhrH6oM2T7L6CCXncE-jksWZ7h~PXgRiy3p4AZsJ075h8pg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1709974"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1709974/Bor_Katk%C4%B1l%C4%B1_Nanofiberlerin_Elektrospinleme_Y%C3%B6ntemi_%C4%B0le_Eldesi"><img alt="Research paper thumbnail of Bor Katkılı Nanofiberlerin Elektrospinleme Yöntemi İle Eldesi" class="work-thumbnail" src="https://attachments.academia-assets.com/7503808/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1709974/Bor_Katk%C4%B1l%C4%B1_Nanofiberlerin_Elektrospinleme_Y%C3%B6ntemi_%C4%B0le_Eldesi">Bor Katkılı Nanofiberlerin Elektrospinleme Yöntemi İle Eldesi</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">&quot;Bu çalışmada bor katkılı YBa2Cu3O7 (YBCO) malzemesi elde edilmiştir. YBCO elde etmek için önce s...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">&quot;Bu çalışmada bor katkılı YBa2Cu3O7 (YBCO) malzemesi elde edilmiştir. YBCO elde etmek için önce sol-jel yöntemiyle itriyum, baryum ve bakır asetat sulu çözeltisini, polivinyl alkol (PVA) ile uygun sıcaklıklarda karıştırılarak hazırlanan kompozit polimerin elektrospinlenerek nanofiber yapılar elde edilmiş, nanofiberlerin ısıl işlemden geçirerek süperiletken malzemeler elde etmişlerdir. <br />Çalışmada elde edilen nanofiberlerin iletkenliği dört nokta probu ile ölçülmüş ve bor katkılı polimerin daha fazla iletkenliğe sahip olduğu saptanmıştır. Nanofiberlerin Diferansiyel Tarama Kalorimetresi (DSC) analizinde bor katkısın fiberlerin ısıya karşı dayanıklılığını artırdığı görülmüştür. <br />Taramalı elektron mikroskobu (SEM) görüntülerinden bor katkılı nanofiberlerin çok düzgün şekilde elektrospinlendiği ve fiberlerin üzerinde diğerinde olduğu gibi herhangi bir topaklanma yada boncuklanma olmadığı görülmüştür.&quot;</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b9f5655a8922134cb41b44e95e032d1d" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7503808,&quot;asset_id&quot;:1709974,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7503808/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709974"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709974"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709974; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709974]").text(description); $(".js-view-count[data-work-id=1709974]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709974; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709974']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709974, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b9f5655a8922134cb41b44e95e032d1d" } } $('.js-work-strip[data-work-id=1709974]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709974,"title":"Bor Katkılı Nanofiberlerin Elektrospinleme Yöntemi İle Eldesi","translated_title":"","metadata":{"abstract":"\"Bu çalışmada bor katkılı YBa2Cu3O7 (YBCO) malzemesi elde edilmiştir. YBCO elde etmek için önce sol-jel yöntemiyle itriyum, baryum ve bakır asetat sulu çözeltisini, polivinyl alkol (PVA) ile uygun sıcaklıklarda karıştırılarak hazırlanan kompozit polimerin elektrospinlenerek nanofiber yapılar elde edilmiş, nanofiberlerin ısıl işlemden geçirerek süperiletken malzemeler elde etmişlerdir. \r\nÇalışmada elde edilen nanofiberlerin iletkenliği dört nokta probu ile ölçülmüş ve bor katkılı polimerin daha fazla iletkenliğe sahip olduğu saptanmıştır. Nanofiberlerin Diferansiyel Tarama Kalorimetresi (DSC) analizinde bor katkısın fiberlerin ısıya karşı dayanıklılığını artırdığı görülmüştür. \r\nTaramalı elektron mikroskobu (SEM) görüntülerinden bor katkılı nanofiberlerin çok düzgün şekilde elektrospinlendiği ve fiberlerin üzerinde diğerinde olduğu gibi herhangi bir topaklanma yada boncuklanma olmadığı görülmüştür.\"","location":"II. Ulusal Bor Çalıştayı","more_info":"İ. Uslu, O. Atakol, M.L. Aksu","organization":"BOREN ve ETİ MADEN sponsorluğunda MTA Ankara'da yapılmıştır.","conference_end_date":{"day":18,"month":4,"year":2008,"errors":{}},"conference_start_date":{"day":17,"month":4,"year":2008,"errors":{}}},"translated_abstract":"\"Bu çalışmada bor katkılı YBa2Cu3O7 (YBCO) malzemesi elde edilmiştir. YBCO elde etmek için önce sol-jel yöntemiyle itriyum, baryum ve bakır asetat sulu çözeltisini, polivinyl alkol (PVA) ile uygun sıcaklıklarda karıştırılarak hazırlanan kompozit polimerin elektrospinlenerek nanofiber yapılar elde edilmiş, nanofiberlerin ısıl işlemden geçirerek süperiletken malzemeler elde etmişlerdir. \r\nÇalışmada elde edilen nanofiberlerin iletkenliği dört nokta probu ile ölçülmüş ve bor katkılı polimerin daha fazla iletkenliğe sahip olduğu saptanmıştır. Nanofiberlerin Diferansiyel Tarama Kalorimetresi (DSC) analizinde bor katkısın fiberlerin ısıya karşı dayanıklılığını artırdığı görülmüştür. \r\nTaramalı elektron mikroskobu (SEM) görüntülerinden bor katkılı nanofiberlerin çok düzgün şekilde elektrospinlendiği ve fiberlerin üzerinde diğerinde olduğu gibi herhangi bir topaklanma yada boncuklanma olmadığı görülmüştür.\"","internal_url":"https://www.academia.edu/1709974/Bor_Katk%C4%B1l%C4%B1_Nanofiberlerin_Elektrospinleme_Y%C3%B6ntemi_%C4%B0le_Eldesi","translated_internal_url":"","created_at":"2012-01-08T02:21:47.018-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7503808,"title":"","file_type":"doc","scribd_thumbnail_url":"https://attachments.academia-assets.com/7503808/thumbnails/1.jpg","file_name":"BorII_superilet.doc","download_url":"https://www.academia.edu/attachments/7503808/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Bor_Katkili_Nanofiberlerin_Elektrospinle.doc","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7503808/BorII_superilet.doc?1326017718=\u0026response-content-disposition=attachment%3B+filename%3DBor_Katkili_Nanofiberlerin_Elektrospinle.doc\u0026Expires=1733898196\u0026Signature=YaUhFy6EPN2RtpPSOFoVQ6Q5WqU~PNhZ0rrATu-~GPmiRT~D6QfBrYH8QmKufpeYN4zDCvQFUqrZhAiXPclJp5Sd191mQ04JCgqApCf1lRHl2Mi2GR-NIAJc6hkuytdRXq1p0LvfeM70gat2QBHiJeWN26sK4jgkowakL5U-jZhVXE9J26Zjz34dEIxSJLdV-tj8y-lU6GKoAL6t3~-yfsNfwJ1mdkx8BnIXm2zEx~INxOE~YF8eGGltHmVCTIEyNJgRV-VVlPmVcAYJr7yS7TImCVp8gLK4IfTbBfr-nofHPSOqjlqZ3R4R6xfvI9jjmRrZNmFGKUgFH1z0rA5oxA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Bor_Katkılı_Nanofiberlerin_Elektrospinleme_Yöntemi_İle_Eldesi","translated_slug":"","page_count":7,"language":"tr","content_type":"Work","summary":"\"Bu çalışmada bor katkılı YBa2Cu3O7 (YBCO) malzemesi elde edilmiştir. YBCO elde etmek için önce sol-jel yöntemiyle itriyum, baryum ve bakır asetat sulu çözeltisini, polivinyl alkol (PVA) ile uygun sıcaklıklarda karıştırılarak hazırlanan kompozit polimerin elektrospinlenerek nanofiber yapılar elde edilmiş, nanofiberlerin ısıl işlemden geçirerek süperiletken malzemeler elde etmişlerdir. \r\nÇalışmada elde edilen nanofiberlerin iletkenliği dört nokta probu ile ölçülmüş ve bor katkılı polimerin daha fazla iletkenliğe sahip olduğu saptanmıştır. Nanofiberlerin Diferansiyel Tarama Kalorimetresi (DSC) analizinde bor katkısın fiberlerin ısıya karşı dayanıklılığını artırdığı görülmüştür. \r\nTaramalı elektron mikroskobu (SEM) görüntülerinden bor katkılı nanofiberlerin çok düzgün şekilde elektrospinlendiği ve fiberlerin üzerinde diğerinde olduğu gibi herhangi bir topaklanma yada boncuklanma olmadığı görülmüştür.\"","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":7503808,"title":"","file_type":"doc","scribd_thumbnail_url":"https://attachments.academia-assets.com/7503808/thumbnails/1.jpg","file_name":"BorII_superilet.doc","download_url":"https://www.academia.edu/attachments/7503808/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Bor_Katkili_Nanofiberlerin_Elektrospinle.doc","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7503808/BorII_superilet.doc?1326017718=\u0026response-content-disposition=attachment%3B+filename%3DBor_Katkili_Nanofiberlerin_Elektrospinle.doc\u0026Expires=1733898196\u0026Signature=YaUhFy6EPN2RtpPSOFoVQ6Q5WqU~PNhZ0rrATu-~GPmiRT~D6QfBrYH8QmKufpeYN4zDCvQFUqrZhAiXPclJp5Sd191mQ04JCgqApCf1lRHl2Mi2GR-NIAJc6hkuytdRXq1p0LvfeM70gat2QBHiJeWN26sK4jgkowakL5U-jZhVXE9J26Zjz34dEIxSJLdV-tj8y-lU6GKoAL6t3~-yfsNfwJ1mdkx8BnIXm2zEx~INxOE~YF8eGGltHmVCTIEyNJgRV-VVlPmVcAYJr7yS7TImCVp8gLK4IfTbBfr-nofHPSOqjlqZ3R4R6xfvI9jjmRrZNmFGKUgFH1z0rA5oxA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="1709972"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/1709972/Preparation_of_PVA_Zinc_Acetate_Composite_Fibers_and_their_Characterization"><img alt="Research paper thumbnail of Preparation of PVA/ Zinc Acetate Composite Fibers and their Characterization" class="work-thumbnail" src="https://attachments.academia-assets.com/7503750/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/1709972/Preparation_of_PVA_Zinc_Acetate_Composite_Fibers_and_their_Characterization">Preparation of PVA/ Zinc Acetate Composite Fibers and their Characterization</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this study the precursor solutions were prepared by dissolving various amounts (4, 8 and 12g) ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this study the precursor solutions were prepared by dissolving various amounts (4, 8 and 12g) of Zn acetate in distilled water. 15g PVA powder dissolved in water to obtain %10 wt solution and 40ml of this aqueous PVA solution was added slowly dropwise into the zinc acetate solution and it was stirred for 3h. Then they were kept in a constant temperature bath at 50 0C for 6h for the reaction occurs between PVA and Zn acetate solution. This precursor solution was taken into a syringe and spinned under 10-20kV with a distence of about 13 cm.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4f1cb596abdb29ef45a590e80cb7a069" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7503750,&quot;asset_id&quot;:1709972,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7503750/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709972"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709972"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709972; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709972]").text(description); $(".js-view-count[data-work-id=1709972]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709972; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709972']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709972, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "4f1cb596abdb29ef45a590e80cb7a069" } } $('.js-work-strip[data-work-id=1709972]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709972,"title":"Preparation of PVA/ Zinc Acetate Composite Fibers and their Characterization","translated_title":"","metadata":{"abstract":"In this study the precursor solutions were prepared by dissolving various amounts (4, 8 and 12g) of Zn acetate in distilled water. 15g PVA powder dissolved in water to obtain %10 wt solution and 40ml of this aqueous PVA solution was added slowly dropwise into the zinc acetate solution and it was stirred for 3h. 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The paper summarizes all phases in the management of orphan sources from detection to storage.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ee326f8859577efb8705e4d382ae83ad" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7407035,&quot;asset_id&quot;:1709350,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7407035/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709350"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709350"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709350; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709350]").text(description); $(".js-view-count[data-work-id=1709350]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709350; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709350']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709350, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "ee326f8859577efb8705e4d382ae83ad" } } $('.js-work-strip[data-work-id=1709350]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709350,"title":"ISSUES IN THE MANAGEMENT OF ORPHAN SOURCES","translated_title":"","metadata":{"abstract":"In recent years, the number of incidents with orphan sources has been constantly increasing, with sources being found not only at customs border controls but also frequently in scrap and in other unexpected locations, thereby giving rise to growing social concern in view of the risks involved. 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Management of these radioactive wastes is briefly described in this paper. Moreover, delay and decay tank systems that are used to collect and store the low level radioactive wastes as a part of low-level radioactive effluent discharge policy are introduced.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="90e27ec98c7039fa1aee195d8cbc3afb" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7406197,&quot;asset_id&quot;:1709348,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7406197/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709348"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709348"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709348; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709348]").text(description); $(".js-view-count[data-work-id=1709348]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709348; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709348']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709348, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "90e27ec98c7039fa1aee195d8cbc3afb" } } $('.js-work-strip[data-work-id=1709348]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709348,"title":"LOW LEVEL RADIOACTIVE WASTE MANAGEMENT AND DISCHARGE POLICIES IN TURKEY","translated_title":"","metadata":{"abstract":"The legal infrastructure in Turkey for the management of low-level radioactive waste covers the liquid, solid and gaseous wastes. 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The response to a radiological emergency may involve many organizations. Therefore, in order to be effective, the response to a radiological emergency must be well co-ordinated, and arrangements must be appropriately integrated with those for a conventional emergency. The regulatory body should require that the emergency arrangements be tested in an exercise before the commencement of operations.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="cad9d242ed19a6e35d11d1a6c507ca93" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7407406,&quot;asset_id&quot;:1709352,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7407406/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709352"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709352"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709352; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709352]").text(description); $(".js-view-count[data-work-id=1709352]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709352; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709352']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709352, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "cad9d242ed19a6e35d11d1a6c507ca93" } } $('.js-work-strip[data-work-id=1709352]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709352,"title":"Security of Radioactive Sources","translated_title":"","metadata":{"abstract":"A State should have a plan ready for response to the detection or suspicion of illicit trafficking in or loss of control of radioactive sources. 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The regulatory body should require that the emergency arrangements be tested in an exercise before the commencement of operations.","more_info":"Ibrahim Uslu (Invited Speaker), Ediz Tanker","organization":"INTERNATIONAL CONFERENCE HELD IN VIENNA,AUSTRIA, 10–13 MARCH 2003, ORGANIZED BY THE INTERNATIONAL ATOMIC ENERGY AGENCY, HOSTED BY THE GOVERNMENT OF AUSTRIA,CO-SPONSORED BY THE GOVERNMENT OF THE RUSSIAN FEDERATION AND THE GOVERNMENT OF THE UNITED STATES OF AMERICA,AND IN CO-OPERATION WITH THE EUROPEAN COMMISSION, THE EUROPEAN POLICE OFFICE, THE INTERNATIONAL CRIMINAL POLICE ORGANIZATION AND THE WORLD CUSTOMS ORGANIZATION","conference_end_date":{"day":13,"month":3,"year":2003,"errors":{}},"conference_start_date":{"day":10,"month":3,"year":2003,"errors":{}}},"translated_abstract":"A State should have a plan ready for response to the detection or suspicion of illicit trafficking in or loss of control of radioactive sources. 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The paper gives detailed information about the discharge policies and radioactive waste tank systems, and dose assessment. Liquid radioavtive waste tank systems, as best available technique, are used to collect and store the low level radioactive wastes and as a part of low level radioactive wastes<br />effluent dischared policy, this decay and delay systems are effectively used for biomedical radioactive wastes generated in hospitals. The decayed waste is then discharged to sewage system in accordance with the discharge limit given in the legislation. Dose assessment studies were also completed and the annual effective dose that would be received by the workers of the waste treatment facility was calculated and the results are presented</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e600c90a4a4d92e26a0357f5e320af18" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:7409541,&quot;asset_id&quot;:1709356,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/7409541/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="1709356"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="1709356"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1709356; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1709356]").text(description); $(".js-view-count[data-work-id=1709356]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1709356; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='1709356']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 1709356, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "e600c90a4a4d92e26a0357f5e320af18" } } $('.js-work-strip[data-work-id=1709356]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":1709356,"title":"Discharge Policies for Low Level Radioactive Effluents in Turkey","translated_title":"","metadata":{"abstract":"The legal infrastructure established in Turkey covers the ways to manage low-level radiaoactive wastes including liquid, solid and gaseous wastes. 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Dose assessment studies were also completed and the annual effective dose that would be received by the workers of the waste treatment facility was calculated and the results are presented","internal_url":"https://www.academia.edu/1709356/Discharge_Policies_for_Low_Level_Radioactive_Effluents_in_Turkey","translated_internal_url":"","created_at":"2012-01-02T23:05:43.830-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"talk","co_author_tags":[],"downloadable_attachments":[{"id":7409541,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/7409541/thumbnails/1.jpg","file_name":"Stockholm.pdf","download_url":"https://www.academia.edu/attachments/7409541/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Discharge_Policies_for_Low_Level_Radioac.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/7409541/Stockholm-libre.pdf?1390851328=\u0026response-content-disposition=attachment%3B+filename%3DDischarge_Policies_for_Low_Level_Radioac.pdf\u0026Expires=1733898196\u0026Signature=gvLgCvmvmHlhgHmOgX9qNHASeRVGHYSSUa0tTc5TtypL00XnE0B2aKF9rKiUpDbb~p7WTOvaLWt2R3JamMuKK6zi-haBsVLe6160XHMGD9132ikli9EWb9eROLHVWloygVTmVgrlHza7K2QP5ti2xDoQlluahRlS581ENqENO9-eY79z8DBh~n~JIttAvmvUcvLmIURBVFYNpwvh0n-9x4Z1IBIel2XtuEoayjVqrywreRaZPpbRkmo6o3MC4oRdYYBNeHj2rNkQ-AQQtxifYoiyUezT~IVP59Gfm0NxB48y3GnH~Ec7oNyXvhu4cxniqZ-DDXO99s70iRd4PZV64Q__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Discharge_Policies_for_Low_Level_Radioactive_Effluents_in_Turkey","translated_slug":"","page_count":9,"language":"en","content_type":"Work","summary":"The legal infrastructure established in Turkey covers the ways to manage low-level radiaoactive wastes including liquid, solid and gaseous wastes. The paper gives detailed information about the discharge policies and radioactive waste tank systems, and dose assessment. Liquid radioavtive waste tank systems, as best available technique, are used to collect and store the low level radioactive wastes and as a part of low level radioactive wastes\neffluent dischared policy, this decay and delay systems are effectively used for biomedical radioactive wastes generated in hospitals. The decayed waste is then discharged to sewage system in accordance with the discharge limit given in the legislation. 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Çalışma koşullarının güvenliği ve özellikle de laboratuvar koşullarının güvenliği, radyasyon ve radyolojik açıdan güvenlik ve ALARA PRENSİBİ, enfeksiyon ve çeşitli hastalıklara karşı sağlık açıdan güvenlik ile çalışma koşulları açıdan daha sağlıklı nasıl çalışılmalı konuları ele alınmıştır. Bu konuda belkide ilk kez hazırlanmış bu sunumun ilginizi çekeceğini düşünüyorum. Bu sunum 7 aralık 2017 tarihinde saat 19 da M.E.G.A SÜREKLİ VE ÜCRETSİZ EĞİTİMLER 6.OTURUMunda Diş hekimlerine anlatılmıştır. Sunumun adı DİŞ HEKİMLİĞİNDE İŞ SAĞLIĞI VE İŞ GÜVENLİĞİ olarak belirlenmiştir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="06d5f9f02c5828cf55981df1cd76b9d7" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:55315416,&quot;asset_id&quot;:35453547,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/55315416/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="35453547"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="35453547"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 35453547; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=35453547]").text(description); $(".js-view-count[data-work-id=35453547]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 35453547; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='35453547']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 35453547, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "06d5f9f02c5828cf55981df1cd76b9d7" } } $('.js-work-strip[data-work-id=35453547]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":35453547,"title":"Dis Hekimlerinin Sagligi ve Guvenligi","translated_title":"","metadata":{"abstract":"Bu sunumda diş hekimlerinin çalışma koşulları ve daha sağlıklı ve güvenli nasıl çalışmaları gerektiği ele alınmıştır. temel olarak üç unsur ele alınmıştır. Çalışma koşullarının güvenliği ve özellikle de laboratuvar koşullarının güvenliği, radyasyon ve radyolojik açıdan güvenlik ve ALARA PRENSİBİ, enfeksiyon ve çeşitli hastalıklara karşı sağlık açıdan güvenlik ile çalışma koşulları açıdan daha sağlıklı nasıl çalışılmalı konuları ele alınmıştır. Bu konuda belkide ilk kez hazırlanmış bu sunumun ilginizi çekeceğini düşünüyorum. Bu sunum 7 aralık 2017 tarihinde saat 19 da M.E.G.A SÜREKLİ VE ÜCRETSİZ EĞİTİMLER 6.OTURUMunda Diş hekimlerine anlatılmıştır. Sunumun adı DİŞ HEKİMLİĞİNDE İŞ SAĞLIĞI VE İŞ GÜVENLİĞİ olarak belirlenmiştir. "},"translated_abstract":"Bu sunumda diş hekimlerinin çalışma koşulları ve daha sağlıklı ve güvenli nasıl çalışmaları gerektiği ele alınmıştır. temel olarak üç unsur ele alınmıştır. Çalışma koşullarının güvenliği ve özellikle de laboratuvar koşullarının güvenliği, radyasyon ve radyolojik açıdan güvenlik ve ALARA PRENSİBİ, enfeksiyon ve çeşitli hastalıklara karşı sağlık açıdan güvenlik ile çalışma koşulları açıdan daha sağlıklı nasıl çalışılmalı konuları ele alınmıştır. Bu konuda belkide ilk kez hazırlanmış bu sunumun ilginizi çekeceğini düşünüyorum. Bu sunum 7 aralık 2017 tarihinde saat 19 da M.E.G.A SÜREKLİ VE ÜCRETSİZ EĞİTİMLER 6.OTURUMunda Diş hekimlerine anlatılmıştır. Sunumun adı DİŞ HEKİMLİĞİNDE İŞ SAĞLIĞI VE İŞ GÜVENLİĞİ olarak belirlenmiştir. 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class="js-work-strip profile--work_container" data-work-id="35447089"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/35447089/Ince_Film_Kaplamada_Kopartma_Sputtering_Yontemi"><img alt="Research paper thumbnail of Ince Film Kaplamada Kopartma (Sputtering) Yontemi" class="work-thumbnail" src="https://attachments.academia-assets.com/55308450/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/35447089/Ince_Film_Kaplamada_Kopartma_Sputtering_Yontemi">Ince Film Kaplamada Kopartma (Sputtering) Yontemi</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">İnce film üretim teknikleri Kopartma (Sputtering) yöntemi Kopartma (Sputtering) sisteminin temel ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">İnce film üretim teknikleri<br />Kopartma (Sputtering) yöntemi<br />Kopartma (Sputtering) sisteminin temel bileşenleri<br />Kopartma (Sputtering) yönteminin parametreleri<br />Kopartma (Sputtering) sisteminin çalışma prensibi<br />Kopartma (Sputtering) yönteminin uygulandığı sistemler<br />Magnetron kopartma (sputtering) sistemi<br />DC/RF (diyot) kopartma (sputtering) sistemi<br />Triyod kopartma (sputtering) sistemi<br />İyon Demeti kopartma (sputtering) Sistemi<br />Magnetron ve magnetron olmayan kopartma sistemleri arasındaki fark<br />Kullanılan gazlar<br />Uygulama alanları<br />Avantajları<br />Dezavantajları<br />Özet<br />Kaynaklar<br />Teşekkür</span></div><div class="wp-workCard_item 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class="js-work-more-abstract-truncated">CVD Tanımı CVD Çalışma Prensibi CVD Reaksiyon Türleri CVD Kullanım Alanları, Örnekleri, Avantajla...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">CVD Tanımı<br />CVD Çalışma Prensibi<br />CVD Reaksiyon Türleri<br />CVD Kullanım Alanları, Örnekleri, Avantajları ve Dezavantajları<br />CVD Çeşitleri<br />CVD ile ALD &amp; PVD Farkları</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="695e737ac72f32004e434f4872c8ceeb" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" 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text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/23661190/Y%C3%BCzey_gerilimi_ve_K%C4%B1lcall%C4%B1k">Yüzey gerilimi ve Kılcallık</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Suda koşan kertenkeleler bunu nasıl başarırlar?Suda yürüyebilen canlılar, Yüzey Gerilimi • Su yüz...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Suda koşan kertenkeleler bunu nasıl başarırlar?Suda yürüyebilen canlılar, Yüzey Gerilimi • Su yüzeyini terk ederken saçlarımızı başımıza yapıştıran etki nedir? Sulu boya fırçasını sudan çıkarırken teller birbirine niçin yapışır?<br />13. Prof.Dr. İbrahim USLU Yüzey Gerilimi • Bir sıvı içindeki molekül diğer moleküller tarafından sarılmış olduğundan her yöne doğru eşit olarak çekilir. Daha düşük enerjilidir. • Ancak yüzeydeki molekül için durum farklıdır. Her yönde çekilmediklerinden yüksek enerjili bu durumda, daha düşük enerjili olma isteği oluşur. • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir.<br /> bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir • Bu içe doğru çekilim yüzünden sıvı en küçük yüzey alanına sahip olacak şekilde büzülür. • Belli bir hacım için en küçük yüzey alanına sahip olan geometrik şekil küre olduğundan bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir.<br />Yüzey Gerilimi • Bir sıvı yüzeyinin neden gergin ve esnek bir zar gibi davrandığı, sıvı yüzeyindeki moleküllere etki eden kohezyon kuvveti ile açıklanabilir. • Bir sıvının özellikleri moleküller arası kuvvetler hesaba katmadan anlaşılamaz. Bu kuvvetlerin varlığı sonucu sıvının gaz haline geçmesi zorlaşır.<br />Bir sıvı içindeki A molekülüne, bu molekülü çevreleyen diğer moleküller tarafından kohezyon kuvvetleri uygulanır. Şekildeki zıt yönlü kuvvetler birbirinin etkisini yok ederek A molekülüne etki eden net kuvvet sıfır olur ve molekül dengede kalır. • Şimdi de sıvı yüzeyine çok yakın bir B molekülü düşünelim. Bütün doğrultulardaki yatay çekim kuvvetleri birbirini dengelediği haldeT B molekülüne etki eden; sıvı içerisine doğru yönelmiş bir F bileşke kuvveti vardır.<br />Mümkün olan en küçük yüzey • Bu kuvvetler sıvı yüzeyindeki B molekülü gibi molekülleri sıvının içine doğru hareket ettirmeğe çalışacaklardır. Bundan dolayı sıvı yüzeyi büzülmek isteyecek ve mümkün olan en küçük yüzeyi alacaktır.<br />Sıvıların En küçük yüzey alanına sahip olma isteği • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir. • Bu durum yüzeyde bir molekül zarı meydana getirir. Oluşan bu zar sıvının içinden dışarı çıkacak ve dışından içine girecek herhangi bir cisme veya taneciğe bir direnç gösterir. Bu dirence, sıvının yüzey gerilimi denir.<br />Yüzey Gerilimi Tanımı • Sıvı yüzeyinin bir hat boyunca kesilmesi durumunda iki yüzey parçasını bir arada tutmak için bir kuvvet uygulanmalıdır . • Yüzey Gerilimi bir sıvının yüzey alanını azaltmaya çalışan kuvvete verilen isimdir. • Bu sıvı üzerindeki 1 cm uzunluğa dik ve sıvı yüzeyine teğet olan kuvvete “yüzey gerilimi “ Çözelti ve yüzey gerilimi • Saf bir madde içerisinde bir madde çözünüyorsa çözünen maddenin ve çözücünün karakterine bağlı olarak yüzey geriliminin değiştiği gözlenmiştir.<br />Soğuk ve sıcak çorbanın tadı nasıl değişir? • Suyun yüzey gerilimi diğer yaygın sıvılarınkinden daha yüksektir. • Saf su, sabun eklenmiş sudan daha fazla yüzey gerilimine sahiptir. Aynı şey yağ katılmış su içinde geçerlidir. Yağ soğuk sudan daha az bir gerilime sahiptir dolayısıyla tüm su yüzeyi üzerinde ince bir tabaka kaplar. • Fakat sıcak su soğuk sudan daha az bir yüzey gerilimine sahiptir çünkü daha hızlı hareket eden moleküllerde kohezyon etkisi daha zayıftır. Bu yağın sıcak çorbada küçük baloncuklar halinde yüzmesini sağlar. • Çorbamız soğuyunca suyun yüzey gerilimi artar ve yağ çorba yüzeyine çekilir ve çorba “yağlı” olur. Sıcak çorba ile soğuğun farklı tat vermesinin temel sebebi suyun yüzey geriliminin sıcaklığa bağlı olmasıdır.<br />Çözeltilerin Yüzey Gerilimi • Çözünen tanecikler içteki çözücü moleküllerinin yüzeydeki çözücü moleküllerini içe doğru çekmesini belli ölçüde engellediğinden çözeltilerin yüzey gerilimi saf çözücüye göre genellikle düşüktür. • Çözücünün yüzey gerilimini düşüren maddeler yüzey aktif, değiştirmeyenler ise yüzey inaktif olarak isimlendirilmektedir. Sulu çözeltiler için yüzey aktif maddeleri; organik asitler, alkoller, esterler, eterler,aminler ve ketonlar şeklinde; yüzey inaktif maddeleri ise inorganik elektrolitler,organik asitlerin tuzları, molar kütleleri küçük olan bazlar yanında şeker ve gliserin gibi uçucu ve elektrolit olmayan maddeler şeklinde sıralayabiliriz.<br />Çözeltilerin Yüzey Gerilimi • Yağ asitleri gibi suyun yüzey gerilimini önemli ölçüde düşüren maddeler, hem polar hidrofilik (su seven) grup hem de apolar hidrofobik (su sevmeyen)grup ihtiva ederler. • Yağ asitlerindeki –COOH grubu gibi hidrofilik gruplar, eğer molekülün kalan apolar kısmı çok büyük değilse, molekülün çözünürlüğünü arttırır. • Yağ asitlerinin hidrokarbon kısımları bir sulu çözeltinin iç kısımlarında rahatsızlık duyarlar (yani yüksek bir serbest enerjiye sahiptirler) ve onlar sıvının iç kısmından yüzeye getirmek çok az iş gerektirir. • Bu sebeple yüzey gerilimini düşüren bir çözünen (yüzey aktif madde), çözeltinin yüzey tabakalarında birikir. • Böyle çözünenlerin ara yüzeyde “pozitif adsorblandığı” söylenir.<br />Tuz Yüzey Gerilimini Etkiler mi? • İyonik tuzlar, genellikle sulu çözeltilerin yüzey gerilimini saf suya göre arttırırlar. • Çözünmüş iyonların yüzey gerilimini yükseltmesinin sebebi, bu iyonlarla su molekülleri arasında meydana gelen iyon- dipol etkileşimlerinin sonucu olarak, su moleküllerinin çözeltinin iç kısımlarına doğru çekilmesidir. • Bu sebeple yeni yüzey oluşturmak için elektrostatik kuvvetlere karşı ilave iş yapılması gerekir. • Böyle çözeltilerde yüzey tabakaları çözünen maddece daha fakirdir. • Yani çözünen madde, yüzey yerine çözeltinin iç kısımlarında toplanır. Bu gibi hallerde çözünenin “negatif adsorblandığı” söylenir.<br />Deniz dalgaları kıyıya vururken niçin köpürür • Saf bir madde içerisinde bir başka madde çözünüyorsa, çözünen maddenin ve çözücünün yapısına bağlı olarak yüzey geriliminin değiştiği gözlenir. • Mesela tuz, suyun yüzey gerilimini azaltır. Tuz, su tanecikleri arasındaki bağları zayıflattığından aralarındaki kohezyon kuvveti, dolayısıyla da yüzey gerilimi azalmış olur. • Bu sebepten deniz dalgaları kıyıya vururken köpürür.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6e801015f9171c788932ea125b755ed5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:44067878,&quot;asset_id&quot;:23661190,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/44067878/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="23661190"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="23661190"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 23661190; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=23661190]").text(description); $(".js-view-count[data-work-id=23661190]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 23661190; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='23661190']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 23661190, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "6e801015f9171c788932ea125b755ed5" } } $('.js-work-strip[data-work-id=23661190]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":23661190,"title":"Yüzey gerilimi ve Kılcallık","translated_title":"","metadata":{"abstract":"Suda koşan kertenkeleler bunu nasıl başarırlar?Suda yürüyebilen canlılar, Yüzey Gerilimi • Su yüzeyini terk ederken saçlarımızı başımıza yapıştıran etki nedir? Sulu boya fırçasını sudan çıkarırken teller birbirine niçin yapışır?\n13. Prof.Dr. İbrahim USLU Yüzey Gerilimi • Bir sıvı içindeki molekül diğer moleküller tarafından sarılmış olduğundan her yöne doğru eşit olarak çekilir. Daha düşük enerjilidir. • Ancak yüzeydeki molekül için durum farklıdır. Her yönde çekilmediklerinden yüksek enerjili bu durumda, daha düşük enerjili olma isteği oluşur. • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir.\n bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir • Bu içe doğru çekilim yüzünden sıvı en küçük yüzey alanına sahip olacak şekilde büzülür. • Belli bir hacım için en küçük yüzey alanına sahip olan geometrik şekil küre olduğundan bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir.\nYüzey Gerilimi • Bir sıvı yüzeyinin neden gergin ve esnek bir zar gibi davrandığı, sıvı yüzeyindeki moleküllere etki eden kohezyon kuvveti ile açıklanabilir. • Bir sıvının özellikleri moleküller arası kuvvetler hesaba katmadan anlaşılamaz. Bu kuvvetlerin varlığı sonucu sıvının gaz haline geçmesi zorlaşır.\nBir sıvı içindeki A molekülüne, bu molekülü çevreleyen diğer moleküller tarafından kohezyon kuvvetleri uygulanır. Şekildeki zıt yönlü kuvvetler birbirinin etkisini yok ederek A molekülüne etki eden net kuvvet sıfır olur ve molekül dengede kalır. • Şimdi de sıvı yüzeyine çok yakın bir B molekülü düşünelim. Bütün doğrultulardaki yatay çekim kuvvetleri birbirini dengelediği haldeT B molekülüne etki eden; sıvı içerisine doğru yönelmiş bir F bileşke kuvveti vardır.\nMümkün olan en küçük yüzey • Bu kuvvetler sıvı yüzeyindeki B molekülü gibi molekülleri sıvının içine doğru hareket ettirmeğe çalışacaklardır. Bundan dolayı sıvı yüzeyi büzülmek isteyecek ve mümkün olan en küçük yüzeyi alacaktır.\nSıvıların En küçük yüzey alanına sahip olma isteği • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir. • Bu durum yüzeyde bir molekül zarı meydana getirir. Oluşan bu zar sıvının içinden dışarı çıkacak ve dışından içine girecek herhangi bir cisme veya taneciğe bir direnç gösterir. Bu dirence, sıvının yüzey gerilimi denir.\nYüzey Gerilimi Tanımı • Sıvı yüzeyinin bir hat boyunca kesilmesi durumunda iki yüzey parçasını bir arada tutmak için bir kuvvet uygulanmalıdır . • Yüzey Gerilimi bir sıvının yüzey alanını azaltmaya çalışan kuvvete verilen isimdir. • Bu sıvı üzerindeki 1 cm uzunluğa dik ve sıvı yüzeyine teğet olan kuvvete “yüzey gerilimi “ Çözelti ve yüzey gerilimi • Saf bir madde içerisinde bir madde çözünüyorsa çözünen maddenin ve çözücünün karakterine bağlı olarak yüzey geriliminin değiştiği gözlenmiştir.\nSoğuk ve sıcak çorbanın tadı nasıl değişir? • Suyun yüzey gerilimi diğer yaygın sıvılarınkinden daha yüksektir. • Saf su, sabun eklenmiş sudan daha fazla yüzey gerilimine sahiptir. Aynı şey yağ katılmış su içinde geçerlidir. Yağ soğuk sudan daha az bir gerilime sahiptir dolayısıyla tüm su yüzeyi üzerinde ince bir tabaka kaplar. • Fakat sıcak su soğuk sudan daha az bir yüzey gerilimine sahiptir çünkü daha hızlı hareket eden moleküllerde kohezyon etkisi daha zayıftır. Bu yağın sıcak çorbada küçük baloncuklar halinde yüzmesini sağlar. • Çorbamız soğuyunca suyun yüzey gerilimi artar ve yağ çorba yüzeyine çekilir ve çorba “yağlı” olur. Sıcak çorba ile soğuğun farklı tat vermesinin temel sebebi suyun yüzey geriliminin sıcaklığa bağlı olmasıdır.\nÇözeltilerin Yüzey Gerilimi • Çözünen tanecikler içteki çözücü moleküllerinin yüzeydeki çözücü moleküllerini içe doğru çekmesini belli ölçüde engellediğinden çözeltilerin yüzey gerilimi saf çözücüye göre genellikle düşüktür. • Çözücünün yüzey gerilimini düşüren maddeler yüzey aktif, değiştirmeyenler ise yüzey inaktif olarak isimlendirilmektedir. Sulu çözeltiler için yüzey aktif maddeleri; organik asitler, alkoller, esterler, eterler,aminler ve ketonlar şeklinde; yüzey inaktif maddeleri ise inorganik elektrolitler,organik asitlerin tuzları, molar kütleleri küçük olan bazlar yanında şeker ve gliserin gibi uçucu ve elektrolit olmayan maddeler şeklinde sıralayabiliriz.\nÇözeltilerin Yüzey Gerilimi • Yağ asitleri gibi suyun yüzey gerilimini önemli ölçüde düşüren maddeler, hem polar hidrofilik (su seven) grup hem de apolar hidrofobik (su sevmeyen)grup ihtiva ederler. • Yağ asitlerindeki –COOH grubu gibi hidrofilik gruplar, eğer molekülün kalan apolar kısmı çok büyük değilse, molekülün çözünürlüğünü arttırır. • Yağ asitlerinin hidrokarbon kısımları bir sulu çözeltinin iç kısımlarında rahatsızlık duyarlar (yani yüksek bir serbest enerjiye sahiptirler) ve onlar sıvının iç kısmından yüzeye getirmek çok az iş gerektirir. • Bu sebeple yüzey gerilimini düşüren bir çözünen (yüzey aktif madde), çözeltinin yüzey tabakalarında birikir. • Böyle çözünenlerin ara yüzeyde “pozitif adsorblandığı” söylenir.\nTuz Yüzey Gerilimini Etkiler mi? • İyonik tuzlar, genellikle sulu çözeltilerin yüzey gerilimini saf suya göre arttırırlar. • Çözünmüş iyonların yüzey gerilimini yükseltmesinin sebebi, bu iyonlarla su molekülleri arasında meydana gelen iyon- dipol etkileşimlerinin sonucu olarak, su moleküllerinin çözeltinin iç kısımlarına doğru çekilmesidir. • Bu sebeple yeni yüzey oluşturmak için elektrostatik kuvvetlere karşı ilave iş yapılması gerekir. • Böyle çözeltilerde yüzey tabakaları çözünen maddece daha fakirdir. • Yani çözünen madde, yüzey yerine çözeltinin iç kısımlarında toplanır. Bu gibi hallerde çözünenin “negatif adsorblandığı” söylenir.\nDeniz dalgaları kıyıya vururken niçin köpürür • Saf bir madde içerisinde bir başka madde çözünüyorsa, çözünen maddenin ve çözücünün yapısına bağlı olarak yüzey geriliminin değiştiği gözlenir. • Mesela tuz, suyun yüzey gerilimini azaltır. Tuz, su tanecikleri arasındaki bağları zayıflattığından aralarındaki kohezyon kuvveti, dolayısıyla da yüzey gerilimi azalmış olur. • Bu sebepten deniz dalgaları kıyıya vururken köpürür.\n"},"translated_abstract":"Suda koşan kertenkeleler bunu nasıl başarırlar?Suda yürüyebilen canlılar, Yüzey Gerilimi • Su yüzeyini terk ederken saçlarımızı başımıza yapıştıran etki nedir? Sulu boya fırçasını sudan çıkarırken teller birbirine niçin yapışır?\n13. Prof.Dr. İbrahim USLU Yüzey Gerilimi • Bir sıvı içindeki molekül diğer moleküller tarafından sarılmış olduğundan her yöne doğru eşit olarak çekilir. Daha düşük enerjilidir. • Ancak yüzeydeki molekül için durum farklıdır. Her yönde çekilmediklerinden yüksek enerjili bu durumda, daha düşük enerjili olma isteği oluşur. • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir.\n bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir • Bu içe doğru çekilim yüzünden sıvı en küçük yüzey alanına sahip olacak şekilde büzülür. • Belli bir hacım için en küçük yüzey alanına sahip olan geometrik şekil küre olduğundan bir sıvı damlası veya sıvı içindeki bir hava kabarcığı daima küresel şekildedir.\nYüzey Gerilimi • Bir sıvı yüzeyinin neden gergin ve esnek bir zar gibi davrandığı, sıvı yüzeyindeki moleküllere etki eden kohezyon kuvveti ile açıklanabilir. • Bir sıvının özellikleri moleküller arası kuvvetler hesaba katmadan anlaşılamaz. Bu kuvvetlerin varlığı sonucu sıvının gaz haline geçmesi zorlaşır.\nBir sıvı içindeki A molekülüne, bu molekülü çevreleyen diğer moleküller tarafından kohezyon kuvvetleri uygulanır. Şekildeki zıt yönlü kuvvetler birbirinin etkisini yok ederek A molekülüne etki eden net kuvvet sıfır olur ve molekül dengede kalır. • Şimdi de sıvı yüzeyine çok yakın bir B molekülü düşünelim. Bütün doğrultulardaki yatay çekim kuvvetleri birbirini dengelediği haldeT B molekülüne etki eden; sıvı içerisine doğru yönelmiş bir F bileşke kuvveti vardır.\nMümkün olan en küçük yüzey • Bu kuvvetler sıvı yüzeyindeki B molekülü gibi molekülleri sıvının içine doğru hareket ettirmeğe çalışacaklardır. Bundan dolayı sıvı yüzeyi büzülmek isteyecek ve mümkün olan en küçük yüzeyi alacaktır.\nSıvıların En küçük yüzey alanına sahip olma isteği • yüzeydeki moleküller içteki moleküllere göre birbirine daha fazla yaklaşır, yüzeyde bir büzülme ve küçülme meydana gelir. • Bu durum yüzeyde bir molekül zarı meydana getirir. Oluşan bu zar sıvının içinden dışarı çıkacak ve dışından içine girecek herhangi bir cisme veya taneciğe bir direnç gösterir. Bu dirence, sıvının yüzey gerilimi denir.\nYüzey Gerilimi Tanımı • Sıvı yüzeyinin bir hat boyunca kesilmesi durumunda iki yüzey parçasını bir arada tutmak için bir kuvvet uygulanmalıdır . • Yüzey Gerilimi bir sıvının yüzey alanını azaltmaya çalışan kuvvete verilen isimdir. • Bu sıvı üzerindeki 1 cm uzunluğa dik ve sıvı yüzeyine teğet olan kuvvete “yüzey gerilimi “ Çözelti ve yüzey gerilimi • Saf bir madde içerisinde bir madde çözünüyorsa çözünen maddenin ve çözücünün karakterine bağlı olarak yüzey geriliminin değiştiği gözlenmiştir.\nSoğuk ve sıcak çorbanın tadı nasıl değişir? • Suyun yüzey gerilimi diğer yaygın sıvılarınkinden daha yüksektir. • Saf su, sabun eklenmiş sudan daha fazla yüzey gerilimine sahiptir. Aynı şey yağ katılmış su içinde geçerlidir. Yağ soğuk sudan daha az bir gerilime sahiptir dolayısıyla tüm su yüzeyi üzerinde ince bir tabaka kaplar. • Fakat sıcak su soğuk sudan daha az bir yüzey gerilimine sahiptir çünkü daha hızlı hareket eden moleküllerde kohezyon etkisi daha zayıftır. Bu yağın sıcak çorbada küçük baloncuklar halinde yüzmesini sağlar. • Çorbamız soğuyunca suyun yüzey gerilimi artar ve yağ çorba yüzeyine çekilir ve çorba “yağlı” olur. Sıcak çorba ile soğuğun farklı tat vermesinin temel sebebi suyun yüzey geriliminin sıcaklığa bağlı olmasıdır.\nÇözeltilerin Yüzey Gerilimi • Çözünen tanecikler içteki çözücü moleküllerinin yüzeydeki çözücü moleküllerini içe doğru çekmesini belli ölçüde engellediğinden çözeltilerin yüzey gerilimi saf çözücüye göre genellikle düşüktür. • Çözücünün yüzey gerilimini düşüren maddeler yüzey aktif, değiştirmeyenler ise yüzey inaktif olarak isimlendirilmektedir. Sulu çözeltiler için yüzey aktif maddeleri; organik asitler, alkoller, esterler, eterler,aminler ve ketonlar şeklinde; yüzey inaktif maddeleri ise inorganik elektrolitler,organik asitlerin tuzları, molar kütleleri küçük olan bazlar yanında şeker ve gliserin gibi uçucu ve elektrolit olmayan maddeler şeklinde sıralayabiliriz.\nÇözeltilerin Yüzey Gerilimi • Yağ asitleri gibi suyun yüzey gerilimini önemli ölçüde düşüren maddeler, hem polar hidrofilik (su seven) grup hem de apolar hidrofobik (su sevmeyen)grup ihtiva ederler. • Yağ asitlerindeki –COOH grubu gibi hidrofilik gruplar, eğer molekülün kalan apolar kısmı çok büyük değilse, molekülün çözünürlüğünü arttırır. • Yağ asitlerinin hidrokarbon kısımları bir sulu çözeltinin iç kısımlarında rahatsızlık duyarlar (yani yüksek bir serbest enerjiye sahiptirler) ve onlar sıvının iç kısmından yüzeye getirmek çok az iş gerektirir. • Bu sebeple yüzey gerilimini düşüren bir çözünen (yüzey aktif madde), çözeltinin yüzey tabakalarında birikir. • Böyle çözünenlerin ara yüzeyde “pozitif adsorblandığı” söylenir.\nTuz Yüzey Gerilimini Etkiler mi? • İyonik tuzlar, genellikle sulu çözeltilerin yüzey gerilimini saf suya göre arttırırlar. • Çözünmüş iyonların yüzey gerilimini yükseltmesinin sebebi, bu iyonlarla su molekülleri arasında meydana gelen iyon- dipol etkileşimlerinin sonucu olarak, su moleküllerinin çözeltinin iç kısımlarına doğru çekilmesidir. • Bu sebeple yeni yüzey oluşturmak için elektrostatik kuvvetlere karşı ilave iş yapılması gerekir. • Böyle çözeltilerde yüzey tabakaları çözünen maddece daha fakirdir. • Yani çözünen madde, yüzey yerine çözeltinin iç kısımlarında toplanır. Bu gibi hallerde çözünenin “negatif adsorblandığı” söylenir.\nDeniz dalgaları kıyıya vururken niçin köpürür • Saf bir madde içerisinde bir başka madde çözünüyorsa, çözünen maddenin ve çözücünün yapısına bağlı olarak yüzey geriliminin değiştiği gözlenir. • Mesela tuz, suyun yüzey gerilimini azaltır. Tuz, su tanecikleri arasındaki bağları zayıflattığından aralarındaki kohezyon kuvveti, dolayısıyla da yüzey gerilimi azalmış olur. • Bu sebepten deniz dalgaları kıyıya vururken 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/></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/23268567/Ozmoz_ve_kollitler">Ozmoz ve kollitler</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. Sunumda hemen her slaytta animasyonlar vardır. An...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. Sunumda hemen her slaytta animasyonlar vardır. Animasyonlar sayesinde öğrencilerin dersi daha iyi kavrayacağı düşünülmektedir. Türk halkına bir armağan daha.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="bc53d6636528d6934703314a31bd19c5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:43740884,&quot;asset_id&quot;:23268567,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/43740884/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="23268567"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="23268567"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 23268567; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=23268567]").text(description); $(".js-view-count[data-work-id=23268567]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 23268567; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='23268567']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 23268567, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "bc53d6636528d6934703314a31bd19c5" } } $('.js-work-strip[data-work-id=23268567]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":23268567,"title":"Ozmoz ve kollitler","translated_title":"","metadata":{"abstract":"Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. Sunumda hemen her slaytta animasyonlar vardır. Animasyonlar sayesinde öğrencilerin dersi daha iyi kavrayacağı düşünülmektedir. Türk halkına bir armağan daha. "},"translated_abstract":"Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. Sunumda hemen her slaytta animasyonlar vardır. Animasyonlar sayesinde öğrencilerin dersi daha iyi kavrayacağı düşünülmektedir. Türk halkına bir armağan daha. 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Sunumda hemen her slaytta animasyonlar vardır. An...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. Sunumda hemen her slaytta animasyonlar vardır. Animasyonlar sayesinde öğrencilerin dersi daha iyi kavrayacağı düşünülmektedir. Türk halkına bir armağan daha.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="23268553"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="23268553"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 23268553; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=23268553]").text(description); $(".js-view-count[data-work-id=23268553]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 23268553; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='23268553']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 23268553, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=23268553]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":23268553,"title":"Ozmoz ve kollitler","translated_title":"","metadata":{"abstract":"Bu sunumda OZMOZ ve KOLLOİTler anlatılmaktadır. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="3187434"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/3187434/Viskozite_Akmazl%C4%B1k"><img alt="Research paper thumbnail of Viskozite - Akmazlık" class="work-thumbnail" src="https://attachments.academia-assets.com/31073392/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/3187434/Viskozite_Akmazl%C4%B1k">Viskozite - Akmazlık</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Vizkozite yani akmazlık konusu çok önemlidir. Petrol gibi akışkanların petrol boru hatlarından tu...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Vizkozite yani akmazlık konusu çok önemlidir. Petrol gibi akışkanların petrol boru hatlarından tutunda akışkanlar kimya, eczacılık, enerji gibi pek çok alanda karşımıza çıkmaktadır. Öğrencilere bu konunun çok iyi anlatılması ve anlatımda görselliğe ve animasyonlara önem verilmesi gerektiğine dair inancımla bu sunumu hazırladım. Ancak maalesef bu sunumumu slideshare.net deki adresimde izlerseniz sunumumdaki animasyonları göremeyeceksiniz. Bu yüzden sunumu <a href="http://gazi.academia.edu/ibrahimUSLU/Teaching-Documents" rel="nofollow">http://gazi.academia.edu/ibrahimUSLU/Teaching-Documents</a> adresimden indirerek izlerseniz tüm animasyonlu hali ile görme şansınız olacaktır. Bilgi paylaşınca güzel, veren el alan elden üstündür.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2728ee13634cf82298fb906532470611" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:31073392,&quot;asset_id&quot;:3187434,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/31073392/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="3187434"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="3187434"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 3187434; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=3187434]").text(description); $(".js-view-count[data-work-id=3187434]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 3187434; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='3187434']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 3187434, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "2728ee13634cf82298fb906532470611" } } $('.js-work-strip[data-work-id=3187434]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":3187434,"title":"Viskozite - Akmazlık","translated_title":"","metadata":{"abstract":"Vizkozite yani akmazlık konusu çok önemlidir. Petrol gibi akışkanların petrol boru hatlarından tutunda akışkanlar kimya, eczacılık, enerji gibi pek çok alanda karşımıza çıkmaktadır. Öğrencilere bu konunun çok iyi anlatılması ve anlatımda görselliğe ve animasyonlara önem verilmesi gerektiğine dair inancımla bu sunumu hazırladım. Ancak maalesef bu sunumumu slideshare.net deki adresimde izlerseniz sunumumdaki animasyonları göremeyeceksiniz. Bu yüzden sunumu http://gazi.academia.edu/ibrahimUSLU/Teaching-Documents adresimden indirerek izlerseniz tüm animasyonlu hali ile görme şansınız olacaktır. Bilgi paylaşınca güzel, veren el alan elden üstündür."},"translated_abstract":"Vizkozite yani akmazlık konusu çok önemlidir. Petrol gibi akışkanların petrol boru hatlarından tutunda akışkanlar kimya, eczacılık, enerji gibi pek çok alanda karşımıza çıkmaktadır. Öğrencilere bu konunun çok iyi anlatılması ve anlatımda görselliğe ve animasyonlara önem verilmesi gerektiğine dair inancımla bu sunumu hazırladım. Ancak maalesef bu sunumumu slideshare.net deki adresimde izlerseniz sunumumdaki animasyonları göremeyeceksiniz. Bu yüzden sunumu http://gazi.academia.edu/ibrahimUSLU/Teaching-Documents adresimden indirerek izlerseniz tüm animasyonlu hali ile görme şansınız olacaktır. 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Petrol gibi akışkanların petrol boru hatlarından tutunda akışkanlar kimya, eczacılık, enerji gibi pek çok alanda karşımıza çıkmaktadır. Öğrencilere bu konunun çok iyi anlatılması ve anlatımda görselliğe ve animasyonlara önem verilmesi gerektiğine dair inancımla bu sunumu hazırladım. Ancak maalesef bu sunumumu slideshare.net deki adresimde izlerseniz sunumumdaki animasyonları göremeyeceksiniz. Bu yüzden sunumu http://gazi.academia.edu/ibrahimUSLU/Teaching-Documents adresimden indirerek izlerseniz tüm animasyonlu hali ile görme şansınız olacaktır. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="287839" id="patents"><div class="js-work-strip profile--work_container" data-work-id="9189934"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/9189934/PRODUCTION_METHOD_OF_BORON_DOPED_LANTANIUM_BISMUTH_OXIDE_NANO_CRYSTALLINE_SOLID_OXIDE_FUEL_CELL_CERAMIC_MATERIAL"><img alt="Research paper thumbnail of PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/9189934/PRODUCTION_METHOD_OF_BORON_DOPED_LANTANIUM_BISMUTH_OXIDE_NANO_CRYSTALLINE_SOLID_OXIDE_FUEL_CELL_CERAMIC_MATERIAL">PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://bilecik.academia.edu/ArdaAytimur">Arda Aytimur</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://selcuk.academia.edu/%C5%9EenolDurmu%C5%9Fo%C4%9Flu">Şenol Durmuşoğlu</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://gazi.academia.edu/ibrahimUSLU">Prof.Dr. İbrahim USLU</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">&quot;This innovation is related to the production of nano crystalline preferably pelleted This innova...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">&quot;This innovation is related to the production of nano crystalline preferably pelleted This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. <br />It enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide.&nbsp; <br />stabilized preferably boron doped bismuth oxide solid oxide fuel cell ceramic material with the use of a polymer solution and electrospinning technique. The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired. <br />This patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures. <br />The polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA). <br />The resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. If carbon is not completely removed and the purity of the resulting material is not at a satisfactory level, the product is subjected to another thermal process preferably at the same temperature and preferably under air atmosphere. The oven can be fed with oxygen gas as desired in order to increase the efficiency of the combustion process and decrease the combustion time. The material can then preferably be grinded and pressed as pellet form.&quot;</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="9189934"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="9189934"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 9189934; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=9189934]").text(description); $(".js-view-count[data-work-id=9189934]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 9189934; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='9189934']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 9189934, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=9189934]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":9189934,"title":"PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL","translated_title":"","metadata":{"abstract":"\"This innovation is related to the production of nano crystalline preferably pelleted This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. \r\nIt enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide. \r\nstabilized preferably boron doped bismuth oxide solid oxide fuel cell ceramic material with the use of a polymer solution and electrospinning technique. The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired. \r\nThis patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures. \r\nThe polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA). \r\nThe resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. If carbon is not completely removed and the purity of the resulting material is not at a satisfactory level, the product is subjected to another thermal process preferably at the same temperature and preferably under air atmosphere. The oven can be fed with oxygen gas as desired in order to increase the efficiency of the combustion process and decrease the combustion time. The material can then preferably be grinded and pressed as pellet form.\"\r\n","more_info":"Patent No: TR 2010 07671 B","publication_date":{"day":21,"month":9,"year":2010,"errors":{}}},"translated_abstract":"\"This innovation is related to the production of nano crystalline preferably pelleted This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. \r\nIt enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide. \r\nstabilized preferably boron doped bismuth oxide solid oxide fuel cell ceramic material with the use of a polymer solution and electrospinning technique. The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired. \r\nThis patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures. \r\nThe polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA). \r\nThe resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. If carbon is not completely removed and the purity of the resulting material is not at a satisfactory level, the product is subjected to another thermal process preferably at the same temperature and preferably under air atmosphere. The oven can be fed with oxygen gas as desired in order to increase the efficiency of the combustion process and decrease the combustion time. 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The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired. \r\nThis patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures. \r\nThe polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA). \r\nThe resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. If carbon is not completely removed and the purity of the resulting material is not at a satisfactory level, the product is subjected to another thermal process preferably at the same temperature and preferably under air atmosphere. The oven can be fed with oxygen gas as desired in order to increase the efficiency of the combustion process and decrease the combustion time. The material can then preferably be grinded and pressed as pellet form.\"\r\n","owner":{"id":981233,"first_name":"Arda","middle_initials":null,"last_name":"Aytimur","page_name":"ArdaAytimur","domain_name":"bilecik","created_at":"2011-11-25T02:29:21.288-08:00","display_name":"Arda Aytimur","url":"https://bilecik.academia.edu/ArdaAytimur"},"attachments":[],"research_interests":[{"id":5596,"name":"Solid Oxide Fuel Cells","url":"https://www.academia.edu/Documents/in/Solid_Oxide_Fuel_Cells"},{"id":58128,"name":"Ceramics","url":"https://www.academia.edu/Documents/in/Ceramics"},{"id":58353,"name":"Nanocrystalline Material","url":"https://www.academia.edu/Documents/in/Nanocrystalline_Material"},{"id":128772,"name":"Lanthanum oxide","url":"https://www.academia.edu/Documents/in/Lanthanum_oxide"},{"id":362531,"name":"Bismuth","url":"https://www.academia.edu/Documents/in/Bismuth"},{"id":1133030,"name":"Nanoceramics","url":"https://www.academia.edu/Documents/in/Nanoceramics"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="3018818"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/3018818/PVA_PAA_H%C4%B0BR%C4%B0T_POL%C4%B0MER_MALZEMELERDEN_YARALARI_TEDAV%C4%B0_ED%C4%B0C%C4%B0_ANT%C4%B0BAKTER%C4%B0YEL_ANALJEZ%C4%B0K_ANT%C4%B0P%C4%B0RET%C4%B0K_VE_ANT%C4%B0ENFLAMATUAR_ETK%C4%B0L%C4%B0_NANOELYAF_YARA_SARGI_MATERYALLER%C4%B0_%C3%9CRET%C4%B0M%C4%B0_VE_Y%C3%96NTEM%C4%B0"><img alt="Research paper thumbnail of PVA/PAA HİBRİT POLİMER MALZEMELERDEN YARALARI TEDAVİ EDİCİ, ANTİBAKTERİYEL, ANALJEZİK, ANTİPİRETİK VE ANTİENFLAMATUAR ETKİLİ NANOELYAF YARA SARGI MATERYALLERİ ÜRETİMİ VE YÖNTEMİ" class="work-thumbnail" src="https://attachments.academia-assets.com/30961400/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/3018818/PVA_PAA_H%C4%B0BR%C4%B0T_POL%C4%B0MER_MALZEMELERDEN_YARALARI_TEDAV%C4%B0_ED%C4%B0C%C4%B0_ANT%C4%B0BAKTER%C4%B0YEL_ANALJEZ%C4%B0K_ANT%C4%B0P%C4%B0RET%C4%B0K_VE_ANT%C4%B0ENFLAMATUAR_ETK%C4%B0L%C4%B0_NANOELYAF_YARA_SARGI_MATERYALLER%C4%B0_%C3%9CRET%C4%B0M%C4%B0_VE_Y%C3%96NTEM%C4%B0">PVA/PAA HİBRİT POLİMER MALZEMELERDEN YARALARI TEDAVİ EDİCİ, ANTİBAKTERİYEL, ANALJEZİK, ANTİPİRETİK VE ANTİENFLAMATUAR ETKİLİ NANOELYAF YARA SARGI MATERYALLERİ ÜRETİMİ VE YÖNTEMİ</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu buluş kısa adı PVA olan polivinil alkol ile kısa adı PAA olan poliakrilik asit hibrit polimer ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu buluş kısa adı PVA olan polivinil alkol ile kısa adı PAA olan poliakrilik asit hibrit polimer malzemelerini kullanarak, antibakteriyel özellik kazandırmak amacıyla tercihen antibiyotik, analjezik, antipiretik ve antienflamatuar özellikler kazandırmak amacıyla tercihen ağrı kesici ve yaraları özellikle yanıkları hızlı bir biçimde tedavi edici özellik kazandırmak için de tercihen aloe vera bitki özünü kullanarak tercihen elektro-eğirme yöntemiyle nanoelyaf yara sargı materyali hazırlama üretimi ve yöntemidir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="75c8b21025441954243e9d79dd3e4bef" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" 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özünü kullanarak tercihen elektro-eğirme yöntemiyle nanoelyaf yara sargı materyali hazırlama üretimi ve 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buluş kısa adı PVA olan polivinil alkol ile kısa adı PAA olan poliakrilik asit hibrit polimer malzemelerini kullanarak, antibakteriyel özellik kazandırmak amacıyla tercihen antibiyotik, analjezik, antipiretik ve antienflamatuar özellikler kazandırmak amacıyla tercihen ağrı kesici ve yaraları özellikle yanıkları hızlı bir biçimde tedavi edici özellik kazandırmak için de tercihen aloe vera bitki özünü kullanarak tercihen elektro-eğirme yöntemiyle nanoelyaf yara sargı materyali hazırlama üretimi ve yöntemidir.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim 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thumbnail of ÇİNKO OKSİT/ALOE VERA KATKILI BİYOPOLİMER BAZLI ANTİMİKROBİYAL ETKİLİ NANOELYAF GIDA AMBALAJ FİLMLERİ ÜRETİMİ VE YÖNTEMİ" class="work-thumbnail" src="https://attachments.academia-assets.com/30961377/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/3018769/%C3%87%C4%B0NKO_OKS%C4%B0T_ALOE_VERA_KATKILI_B%C4%B0YOPOL%C4%B0MER_BAZLI_ANT%C4%B0M%C4%B0KROB%C4%B0YAL_ETK%C4%B0L%C4%B0_NANOELYAF_GIDA_AMBALAJ_F%C4%B0LMLER%C4%B0_%C3%9CRET%C4%B0M%C4%B0_VE_Y%C3%96NTEM%C4%B0">ÇİNKO OKSİT/ALOE VERA KATKILI BİYOPOLİMER BAZLI ANTİMİKROBİYAL ETKİLİ NANOELYAF GIDA AMBALAJ FİLMLERİ ÜRETİMİ VE YÖNTEMİ</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu buluş kısa adı PVA olan polivinil alkol biyobozunur polimer malzemesi kullanarak, ve istendiği...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu buluş kısa adı PVA olan polivinil alkol biyobozunur polimer malzemesi kullanarak, ve istendiğinde kısa adı PEG olan polietilen glikol, kısa adı PVP olan polivinil pirolidon ve kısa adı PLA olan polilaktik asit gibi polimerlerin her birini ve bir kaçını gerektiğinde az miktarda PVA biyobozunur polimeriyle karıştırıp oluşturulan kopolimere, istendiğinde antimikrobiyal etki sağlaması için, bir doğal polimer olan aloe vera ile çinko oksit katkısı sağlanıp söz konusu hibrit polimer çözeltisinin elektro-eğirme yöntemiyle nanoelyaf gıda ambalaj filmleri hazırlama üretimi ve yöntemidir. Yüksek denge bağıl nemine sahip gıdaların nem kaybetmemesi için elektro-eğirilecek polimer malzemesine kısa adı PAA olan poliakrilik asit ilave edilebilir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9f0274b888600d3ac87121312a543902" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:30961377,&quot;asset_id&quot;:3018769,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/30961377/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="3018769"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="3018769"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 3018769; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=3018769]").text(description); $(".js-view-count[data-work-id=3018769]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 3018769; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='3018769']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 3018769, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "9f0274b888600d3ac87121312a543902" } } $('.js-work-strip[data-work-id=3018769]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":3018769,"title":"ÇİNKO OKSİT/ALOE VERA KATKILI BİYOPOLİMER BAZLI ANTİMİKROBİYAL ETKİLİ NANOELYAF GIDA AMBALAJ FİLMLERİ ÜRETİMİ VE YÖNTEMİ","translated_title":"","metadata":{"abstract":"Bu buluş kısa adı PVA olan polivinil alkol biyobozunur polimer malzemesi kullanarak, ve istendiğinde kısa adı PEG olan polietilen glikol, kısa adı PVP olan polivinil pirolidon ve kısa adı PLA olan polilaktik asit gibi polimerlerin her birini ve bir kaçını gerektiğinde az miktarda PVA biyobozunur polimeriyle karıştırıp oluşturulan kopolimere, istendiğinde antimikrobiyal etki sağlaması için, bir doğal polimer olan aloe vera ile çinko oksit katkısı sağlanıp söz konusu hibrit polimer çözeltisinin elektro-eğirme yöntemiyle nanoelyaf gıda ambalaj filmleri hazırlama üretimi ve yöntemidir. Yüksek denge bağıl nemine sahip gıdaların nem kaybetmemesi için elektro-eğirilecek polimer malzemesine kısa adı PAA olan poliakrilik asit ilave edilebilir."},"translated_abstract":"Bu buluş kısa adı PVA olan polivinil alkol biyobozunur polimer malzemesi kullanarak, ve istendiğinde kısa adı PEG olan polietilen glikol, kısa adı PVP olan polivinil pirolidon ve kısa adı PLA olan polilaktik asit gibi polimerlerin her birini ve bir kaçını gerektiğinde az miktarda PVA biyobozunur polimeriyle karıştırıp oluşturulan kopolimere, istendiğinde antimikrobiyal etki sağlaması için, bir doğal polimer olan aloe vera ile çinko oksit katkısı sağlanıp söz konusu hibrit polimer çözeltisinin elektro-eğirme yöntemiyle nanoelyaf gıda ambalaj filmleri hazırlama üretimi ve yöntemidir. 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Yüksek denge bağıl nemine sahip gıdaların nem kaybetmemesi için elektro-eğirilecek polimer malzemesine kısa adı PAA olan poliakrilik asit ilave edilebilir.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":30961377,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/30961377/thumbnails/1.jpg","file_name":"Gida_ambalaj.pdf","download_url":"https://www.academia.edu/attachments/30961377/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"CINKO_OKSIT_ALOE_VERA_KATKILI_BIYOPOLIME.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/30961377/Gida_ambalaj-libre.pdf?1392159992=\u0026response-content-disposition=attachment%3B+filename%3DCINKO_OKSIT_ALOE_VERA_KATKILI_BIYOPOLIME.pdf\u0026Expires=1733898197\u0026Signature=a7PW1AHrcWfGRBx1YycO~F3IqNsI6oTIPrP5oYNpT7bfv3ozyjWS9-TYOcUCsbHAnM1ah9sBFdZOlSuLifNiBcJ8ju34ur1g2fg6WWHmeR7nGBE9YVR0ztnNXY6vHOktrL17yNN9-ERTQFC~tggF02kTiYpuewAWeea6Ax~5xQwR8oICDCfLQHJe61FYqlg8S6kYvhremqFkEft4cEBxdeidiIluUq~3~4b8cJbqvWlujMyQRUGMW8csf1mA4xgeRZI4Paz4PWiivrVSVhDphxqbW3QLNHZk~k43cKlt4nj4JSprrMQjiNLaxjdhI72GHoT~njtGqnXjc5mycUytIw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":377581,"name":"Aloe Vera","url":"https://www.academia.edu/Documents/in/Aloe_Vera"},{"id":673888,"name":"Gıda","url":"https://www.academia.edu/Documents/in/Gida"},{"id":739388,"name":"Ambalaj","url":"https://www.academia.edu/Documents/in/Ambalaj"},{"id":739389,"name":"Gıda Ambalaj","url":"https://www.academia.edu/Documents/in/Gida_Ambalaj"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2028580"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2028580/POL%C4%B0MER_MALZEMELERDEN_D%C3%9C%C5%9E%C3%9CK_SICAKLIKLARDA_BOR_KARB%C3%9CR_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0"><img alt="Research paper thumbnail of POLİMER MALZEMELERDEN DÜŞÜK SICAKLIKLARDA BOR KARBÜR ÜRETİM YÖNTEMİ" class="work-thumbnail" src="https://attachments.academia-assets.com/29751363/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2028580/POL%C4%B0MER_MALZEMELERDEN_D%C3%9C%C5%9E%C3%9CK_SICAKLIKLARDA_BOR_KARB%C3%9CR_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0">POLİMER MALZEMELERDEN DÜŞÜK SICAKLIKLARDA BOR KARBÜR ÜRETİM YÖNTEMİ</a></div><div class="wp-workCard_item"><span>Patent no: TR 2009/02957 (İnceleme aşamasında)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu patent PVA, PEG, PPG gibi polimer malzemeyi ve tercihan borik asit vb bir bor bileşiği belirli...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu patent PVA, PEG, PPG gibi polimer malzemeyi ve tercihan borik asit vb bir bor bileşiği belirli oranlarda karıştırıp reaksiyon ürünü hibrit polimeri 400-700 oC kalsinasyon ve 1000-1600 oC sinterleme işlemine tabi tutarak bor karbür üretim yöntemi ile ilgilidir. Bu yöntemin en büyük özelliği ısıl işlem sırasında isteğe bağlı olarak mikro dalga fırın kullanarak enerjiden ve zamandan büyük tasarruf edilmesini sağlamasıdır. Ayrıca bu yöntemle kalsinasyon sonrası öğütme işleminden sonra pelet aşamasında sinterlenecek malzemeye elementel bor yada borik asit katarak bor karbürün borca daha zengin olması veya aluminyum yada mağnezyum katarak değişik bor karbür alaşımlarının hazırlanması mümkün olabilmektedir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0561610f968fae3b1599bfaa7da35726" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751363,&quot;asset_id&quot;:2028580,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751363/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2028580"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2028580"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2028580; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2028580]").text(description); $(".js-view-count[data-work-id=2028580]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2028580; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2028580']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2028580, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "0561610f968fae3b1599bfaa7da35726" } } $('.js-work-strip[data-work-id=2028580]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2028580,"title":"POLİMER MALZEMELERDEN DÜŞÜK SICAKLIKLARDA BOR KARBÜR ÜRETİM YÖNTEMİ","translated_title":"","metadata":{"abstract":"Bu patent PVA, PEG, PPG gibi polimer malzemeyi ve tercihan borik asit vb bir bor bileşiği belirli oranlarda karıştırıp reaksiyon ürünü hibrit polimeri 400-700 oC kalsinasyon ve 1000-1600 oC sinterleme işlemine tabi tutarak bor karbür üretim yöntemi ile ilgilidir. Bu yöntemin en büyük özelliği ısıl işlem sırasında isteğe bağlı olarak mikro dalga fırın kullanarak enerjiden ve zamandan büyük tasarruf edilmesini sağlamasıdır. Ayrıca bu yöntemle kalsinasyon sonrası öğütme işleminden sonra pelet aşamasında sinterlenecek malzemeye elementel bor yada borik asit katarak bor karbürün borca daha zengin olması veya aluminyum yada mağnezyum katarak değişik bor karbür alaşımlarının hazırlanması mümkün olabilmektedir.","publication_name":"Patent no: TR 2009/02957 (İnceleme aşamasında)"},"translated_abstract":"Bu patent PVA, PEG, PPG gibi polimer malzemeyi ve tercihan borik asit vb bir bor bileşiği belirli oranlarda karıştırıp reaksiyon ürünü hibrit polimeri 400-700 oC kalsinasyon ve 1000-1600 oC sinterleme işlemine tabi tutarak bor karbür üretim yöntemi ile ilgilidir. Bu yöntemin en büyük özelliği ısıl işlem sırasında isteğe bağlı olarak mikro dalga fırın kullanarak enerjiden ve zamandan büyük tasarruf edilmesini sağlamasıdır. Ayrıca bu yöntemle kalsinasyon sonrası öğütme işleminden sonra pelet aşamasında sinterlenecek malzemeye elementel bor yada borik asit katarak bor karbürün borca daha zengin olması veya aluminyum yada mağnezyum katarak değişik bor karbür alaşımlarının hazırlanması mümkün olabilmektedir.","internal_url":"https://www.academia.edu/2028580/POL%C4%B0MER_MALZEMELERDEN_D%C3%9C%C5%9E%C3%9CK_SICAKLIKLARDA_BOR_KARB%C3%9CR_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0","translated_internal_url":"","created_at":"2012-10-14T16:43:41.495-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[{"id":29751363,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751363/thumbnails/1.jpg","file_name":"BOR_KARBUR_POSTER.pdf","download_url":"https://www.academia.edu/attachments/29751363/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"POLIMER_MALZEMELERDEN_DUSUK_SICAKLIKLARD.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751363/BOR_KARBUR_POSTER-libre.pdf?1390877997=\u0026response-content-disposition=attachment%3B+filename%3DPOLIMER_MALZEMELERDEN_DUSUK_SICAKLIKLARD.pdf\u0026Expires=1733756526\u0026Signature=GqiJhz06epBEsGkpAPcobtizOMHa41VTcUzjFv3HCIMihxuBlPHEDPp0WSu5FN78CkVjegEqBPw29CL5isVCs64rPu71ezOCXBInpcgPvPIxaOiOaAPu0lLHAMbtvMAn3UB~d-TmQGyE5Q-V9z5Qk8mRQ9Y6v2AU9Mlg3TuZrgPIBr2HWtI4yekF5e4rPb562RTvSgYtNr-fShyRzcU~tBLxn0VCuErpedw4HrXsXi-IphIBwrOdf4WaRW9DioUbGex6epiV-neMYWLRB0SISZWFy8Ni4r8ig4SuGTkdfdarhzQWjUGFjYdpA58-i~jwabjP7pV1GyUOvxwUZHbCqA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"POLİMER_MALZEMELERDEN_DÜŞÜK_SICAKLIKLARDA_BOR_KARBÜR_ÜRETİM_YÖNTEMİ","translated_slug":"","page_count":1,"language":"tr","content_type":"Work","summary":"Bu patent PVA, PEG, PPG gibi polimer malzemeyi ve tercihan borik asit vb bir bor bileşiği belirli oranlarda karıştırıp reaksiyon ürünü hibrit polimeri 400-700 oC kalsinasyon ve 1000-1600 oC sinterleme işlemine tabi tutarak bor karbür üretim yöntemi ile ilgilidir. 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Chinese Chemical Letters 2009","url":"https://www.academia.edu/Documents/in/M._S._Chinese_Chemical_Letters_2009"},{"id":982308,"name":"Hybrid Polymer Solution","url":"https://www.academia.edu/Documents/in/Hybrid_Polymer_Solution"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2017190"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2017190/B%C4%B0TK%C4%B0SEL_EKSTRELER_%C4%B0%C3%87EREN_HORLAMAYI_TEDAV%C4%B0_ED%C4%B0C%C4%B0_SOL%C3%9CSYON_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0"><img alt="Research paper thumbnail of BİTKİSEL EKSTRELER İÇEREN HORLAMAYI TEDAVİ EDİCİ SOLÜSYON ÜRETİM YÖNTEMİ" class="work-thumbnail" src="https://attachments.academia-assets.com/29751455/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2017190/B%C4%B0TK%C4%B0SEL_EKSTRELER_%C4%B0%C3%87EREN_HORLAMAYI_TEDAV%C4%B0_ED%C4%B0C%C4%B0_SOL%C3%9CSYON_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0">BİTKİSEL EKSTRELER İÇEREN HORLAMAYI TEDAVİ EDİCİ SOLÜSYON ÜRETİM YÖNTEMİ</a></div><div class="wp-workCard_item"><span>Patent no: TR 2010/10399 (İnceleme aşamasında)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu buluş oral yolla, ağız içi dokuları nar kabuğu ekstresi ile sıkılaştırıp, çoğu bitkisel kökenl...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu buluş oral yolla, ağız içi dokuları nar kabuğu ekstresi ile sıkılaştırıp, çoğu bitkisel kökenli doğal maddelerin etkileriyle de dokuların rahatlatılması ve kayganlaştırılmasını sağlayarak, hava akışı engelleyici maddeleri incelterek, horlamayı tedavi etmek üzere hazırlanan gargara ya da sprey formunda solüsyonun üretim yöntemi ile ilgilidir. <br />Bu buluşta da bu dört yaklaşım göz önüne alınarak horlamın tedavisi amaçlanmaktadır. Birincisi, astringent yani doku sıkılaştırıcılar ile söz konusu dokuların yüzeyi sertleştirilmesi, ikincisi ağız içi dokular rahatlatılarak, dokuların titreşimleri sonucu oluşan yara ve tahrişler hafifletilmesi, üçüncüsü çeşitli nedenlerden dolayı ağız içinde oluşan mukus, balgam ve benzeri maddelerin balgam sökücü ajanlarla boğaz ve gırtlaktan uzaklaştırılarak, bu bölgedeki hava akışının rahatlatılması. Dördüncü olarak da, ağız içi dokularının yüzeyi kayganlaştırılarak ve biyoadhesif ajanlar kullanarak bu kayganlaşmayı daha etkin kılıp, böylece solunum sırasında hava sürtünme sonucu oluşan horlamanın önüne geçilmesi. <br />Bu buluşta kullanılan bitkisel uçucu yağlar ve diğer kimyasal maddelerin çoğu aynı zamanda antibakteriyel, antiseptik, ağız kokularını gideren, aft gibi ağızda oluşabilen yaraları tedavi edebilme özelliğine de sahiptir. Bu yüzden horlamayı gidermenin yanı sıra kullanıcıların ağız ve diş sağlığına da ciddi yararlar sağlayacağı açıktır.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="bc1d3d8b664760b5109a8b39b2e609db" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751455,&quot;asset_id&quot;:2017190,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751455/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2017190"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2017190"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2017190; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2017190]").text(description); $(".js-view-count[data-work-id=2017190]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2017190; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2017190']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2017190, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "bc1d3d8b664760b5109a8b39b2e609db" } } $('.js-work-strip[data-work-id=2017190]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2017190,"title":"BİTKİSEL EKSTRELER İÇEREN HORLAMAYI TEDAVİ EDİCİ SOLÜSYON ÜRETİM YÖNTEMİ","translated_title":"","metadata":{"abstract":"Bu buluş oral yolla, ağız içi dokuları nar kabuğu ekstresi ile sıkılaştırıp, çoğu bitkisel kökenli doğal maddelerin etkileriyle de dokuların rahatlatılması ve kayganlaştırılmasını sağlayarak, hava akışı engelleyici maddeleri incelterek, horlamayı tedavi etmek üzere hazırlanan gargara ya da sprey formunda solüsyonun üretim yöntemi ile ilgilidir.\r\nBu buluşta da bu dört yaklaşım göz önüne alınarak horlamın tedavisi amaçlanmaktadır. Birincisi, astringent yani doku sıkılaştırıcılar ile söz konusu dokuların yüzeyi sertleştirilmesi, ikincisi ağız içi dokular rahatlatılarak, dokuların titreşimleri sonucu oluşan yara ve tahrişler hafifletilmesi, üçüncüsü çeşitli nedenlerden dolayı ağız içinde oluşan mukus, balgam ve benzeri maddelerin balgam sökücü ajanlarla boğaz ve gırtlaktan uzaklaştırılarak, bu bölgedeki hava akışının rahatlatılması. Dördüncü olarak da, ağız içi dokularının yüzeyi kayganlaştırılarak ve biyoadhesif ajanlar kullanarak bu kayganlaşmayı daha etkin kılıp, böylece solunum sırasında hava sürtünme sonucu oluşan horlamanın önüne geçilmesi. \r\nBu buluşta kullanılan bitkisel uçucu yağlar ve diğer kimyasal maddelerin çoğu aynı zamanda antibakteriyel, antiseptik, ağız kokularını gideren, aft gibi ağızda oluşabilen yaraları tedavi edebilme özelliğine de sahiptir. Bu yüzden horlamayı gidermenin yanı sıra kullanıcıların ağız ve diş sağlığına da ciddi yararlar sağlayacağı açıktır. \r\n","publication_name":"Patent no: TR 2010/10399 (İnceleme aşamasında)"},"translated_abstract":"Bu buluş oral yolla, ağız içi dokuları nar kabuğu ekstresi ile sıkılaştırıp, çoğu bitkisel kökenli doğal maddelerin etkileriyle de dokuların rahatlatılması ve kayganlaştırılmasını sağlayarak, hava akışı engelleyici maddeleri incelterek, horlamayı tedavi etmek üzere hazırlanan gargara ya da sprey formunda solüsyonun üretim yöntemi ile ilgilidir.\r\nBu buluşta da bu dört yaklaşım göz önüne alınarak horlamın tedavisi amaçlanmaktadır. Birincisi, astringent yani doku sıkılaştırıcılar ile söz konusu dokuların yüzeyi sertleştirilmesi, ikincisi ağız içi dokular rahatlatılarak, dokuların titreşimleri sonucu oluşan yara ve tahrişler hafifletilmesi, üçüncüsü çeşitli nedenlerden dolayı ağız içinde oluşan mukus, balgam ve benzeri maddelerin balgam sökücü ajanlarla boğaz ve gırtlaktan uzaklaştırılarak, bu bölgedeki hava akışının rahatlatılması. Dördüncü olarak da, ağız içi dokularının yüzeyi kayganlaştırılarak ve biyoadhesif ajanlar kullanarak bu kayganlaşmayı daha etkin kılıp, böylece solunum sırasında hava sürtünme sonucu oluşan horlamanın önüne geçilmesi. \r\nBu buluşta kullanılan bitkisel uçucu yağlar ve diğer kimyasal maddelerin çoğu aynı zamanda antibakteriyel, antiseptik, ağız kokularını gideren, aft gibi ağızda oluşabilen yaraları tedavi edebilme özelliğine de sahiptir. Bu yüzden horlamayı gidermenin yanı sıra kullanıcıların ağız ve diş sağlığına da ciddi yararlar sağlayacağı açıktır. \r\n","internal_url":"https://www.academia.edu/2017190/B%C4%B0TK%C4%B0SEL_EKSTRELER_%C4%B0%C3%87EREN_HORLAMAYI_TEDAV%C4%B0_ED%C4%B0C%C4%B0_SOL%C3%9CSYON_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0","translated_internal_url":"","created_at":"2012-10-11T00:34:09.233-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[{"id":29751455,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751455/thumbnails/1.jpg","file_name":"Horlama_poster.pdf","download_url":"https://www.academia.edu/attachments/29751455/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"BITKISEL_EKSTRELER_ICEREN_HORLAMAYI_TEDA.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751455/Horlama_poster-libre.pdf?1390878000=\u0026response-content-disposition=attachment%3B+filename%3DBITKISEL_EKSTRELER_ICEREN_HORLAMAYI_TEDA.pdf\u0026Expires=1733756526\u0026Signature=XyHUsmBStnbxg0x65biXK2AIcBZFn7NVEXMxh~3YvTK-KH8yNW~FI44RF-4WL4M-mi4iFywj9SoxfeztXx9IspfTl4XxIt6TNgTtOzjEUn-EJ1f68CA5TdeLv1xKzQfh7NErU7hLQHl8HbbA9WcFsyUQmLg8TrvNMnLxJjd1t9jvQk893pOVC8MeZ9l9T02u6KKu29G0Mboxb9eBPhAZLjk2VqGvrAX3jKOHmc~OOjrklqOOyKNjtlXaPOaJ-qmUy0LV8-j9X4eyP-uHN6oCkOEj-Od6OxBfUg98TJ3nN1c83efeM-O-JI2XjnECe0QGy1VF~6P2~qA3Zt61WOoP4w__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"BİTKİSEL_EKSTRELER_İÇEREN_HORLAMAYI_TEDAVİ_EDİCİ_SOLÜSYON_ÜRETİM_YÖNTEMİ","translated_slug":"","page_count":1,"language":"tr","content_type":"Work","summary":"Bu buluş oral yolla, ağız içi dokuları nar kabuğu ekstresi ile sıkılaştırıp, çoğu bitkisel kökenli doğal maddelerin etkileriyle de dokuların rahatlatılması ve kayganlaştırılmasını sağlayarak, hava akışı engelleyici maddeleri incelterek, horlamayı tedavi etmek üzere hazırlanan gargara ya da sprey formunda solüsyonun üretim yöntemi ile ilgilidir.\r\nBu buluşta da bu dört yaklaşım göz önüne alınarak horlamın tedavisi amaçlanmaktadır. Birincisi, astringent yani doku sıkılaştırıcılar ile söz konusu dokuların yüzeyi sertleştirilmesi, ikincisi ağız içi dokular rahatlatılarak, dokuların titreşimleri sonucu oluşan yara ve tahrişler hafifletilmesi, üçüncüsü çeşitli nedenlerden dolayı ağız içinde oluşan mukus, balgam ve benzeri maddelerin balgam sökücü ajanlarla boğaz ve gırtlaktan uzaklaştırılarak, bu bölgedeki hava akışının rahatlatılması. Dördüncü olarak da, ağız içi dokularının yüzeyi kayganlaştırılarak ve biyoadhesif ajanlar kullanarak bu kayganlaşmayı daha etkin kılıp, böylece solunum sırasında hava sürtünme sonucu oluşan horlamanın önüne geçilmesi. \r\nBu buluşta kullanılan bitkisel uçucu yağlar ve diğer kimyasal maddelerin çoğu aynı zamanda antibakteriyel, antiseptik, ağız kokularını gideren, aft gibi ağızda oluşabilen yaraları tedavi edebilme özelliğine de sahiptir. Bu yüzden horlamayı gidermenin yanı sıra kullanıcıların ağız ve diş sağlığına da ciddi yararlar sağlayacağı açıktır. \r\n","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":29751455,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751455/thumbnails/1.jpg","file_name":"Horlama_poster.pdf","download_url":"https://www.academia.edu/attachments/29751455/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"BITKISEL_EKSTRELER_ICEREN_HORLAMAYI_TEDA.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751455/Horlama_poster-libre.pdf?1390878000=\u0026response-content-disposition=attachment%3B+filename%3DBITKISEL_EKSTRELER_ICEREN_HORLAMAYI_TEDA.pdf\u0026Expires=1733756526\u0026Signature=XyHUsmBStnbxg0x65biXK2AIcBZFn7NVEXMxh~3YvTK-KH8yNW~FI44RF-4WL4M-mi4iFywj9SoxfeztXx9IspfTl4XxIt6TNgTtOzjEUn-EJ1f68CA5TdeLv1xKzQfh7NErU7hLQHl8HbbA9WcFsyUQmLg8TrvNMnLxJjd1t9jvQk893pOVC8MeZ9l9T02u6KKu29G0Mboxb9eBPhAZLjk2VqGvrAX3jKOHmc~OOjrklqOOyKNjtlXaPOaJ-qmUy0LV8-j9X4eyP-uHN6oCkOEj-Od6OxBfUg98TJ3nN1c83efeM-O-JI2XjnECe0QGy1VF~6P2~qA3Zt61WOoP4w__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":622426,"name":"Snore","url":"https://www.academia.edu/Documents/in/Snore"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2016111"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2016111/PRODUCTION_METHOD_OF_BORON_DOPED_LANTANIUM_BISMUTH_OXIDE_NANO_CRYSTALLINE_SOLID_OXIDE_FUEL_CELL_CERAMIC_MATERIAL"><img alt="Research paper thumbnail of PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL" class="work-thumbnail" src="https://attachments.academia-assets.com/29751499/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2016111/PRODUCTION_METHOD_OF_BORON_DOPED_LANTANIUM_BISMUTH_OXIDE_NANO_CRYSTALLINE_SOLID_OXIDE_FUEL_CELL_CERAMIC_MATERIAL">PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL</a></div><div class="wp-workCard_item"><span>Patent No: TR 2010/07671(İnceleme aşamasında)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">&quot;This innovation is related to the production of nano crystalline preferably pelleted This innova...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">&quot;This innovation is related to the production of nano crystalline preferably pelleted This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. <br />It enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide.&nbsp; <br /> stabilized preferably boron doped bismuth oxide solid oxide fuel cell ceramic material with the use of a polymer solution and electrospinning technique. The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired. <br /> This patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures. <br />The polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA). <br />The resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. If carbon is not completely removed and the purity of the resulting material is not at a satisfactory level, the product is subjected to another thermal process preferably at the same temperature and preferably under air atmosphere. The oven can be fed with oxygen gas as desired in order to increase the efficiency of the combustion process and decrease the combustion time. The material can then preferably be grinded and pressed as pellet form.&quot;</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0abab65162df1ee422c21b0d4f7269b3" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751499,&quot;asset_id&quot;:2016111,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751499/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2016111"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2016111"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2016111; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2016111]").text(description); $(".js-view-count[data-work-id=2016111]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2016111; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2016111']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2016111, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "0abab65162df1ee422c21b0d4f7269b3" } } $('.js-work-strip[data-work-id=2016111]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2016111,"title":"PRODUCTION METHOD OF BORON DOPED LANTANIUM – BISMUTH OXIDE NANO CRYSTALLINE SOLID OXIDE FUEL CELL CERAMIC MATERIAL","translated_title":"","metadata":{"abstract":"\"This innovation is related to the production of nano crystalline preferably pelleted This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. \r\nIt enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide. \r\n stabilized preferably boron doped bismuth oxide solid oxide fuel cell ceramic material with the use of a polymer solution and electrospinning technique. 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The bismuth source is preferably bismuth acetate or bismuth nitrate if desired and lanthanum source is preferably lanthanum acetate or lanthanum nitrate if desired.\r\n\tThis patent involves the addition of boron in order to obtain the ceramic material at lower temperature with the density close to the theoretical value preferably using boric acid as the boron source. This will enable us to obtain high quality hard ceramic composite material resistant against chemical, erosion and elevated temperatures.\r\nThe polymer material to be electrospun are the single or the hybrid or the combined uses of glycol (PEG), polyethylene oxide (PEO), polyvinyl acetate (PVAc), polyvinyl pyrolydine (PVP) and/or polyvinyl alcohol (PVA).\r\nThe resulting electrospun and dry nano- fiber polymer material is calcified at preferably at 800 oC for preferably 2 hours. 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The material can then preferably be grinded and pressed as pellet form.\"","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":29751499,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751499/thumbnails/1.jpg","file_name":"lantan_poster.pdf","download_url":"https://www.academia.edu/attachments/29751499/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"PRODUCTION_METHOD_OF_BORON_DOPED_LANTANI.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751499/lantan_poster-libre.pdf?1390878006=\u0026response-content-disposition=attachment%3B+filename%3DPRODUCTION_METHOD_OF_BORON_DOPED_LANTANI.pdf\u0026Expires=1733898197\u0026Signature=DYB44ZgK71BnJL43gR4nYWegtg6A0BoHcXqWD3ZegaskMeq5IV-sbV1-9fAYv6ERLxMyMc3kUbgB1-dNmSManVGIsNUtBS9EgzP96t36EDlRjbVu1yEglq-68OG-RNWZS~ne6rS6HpE9tuG718I18LS3qMIS~vsqW6n3kxg1GHy6QAovl8PLF96l5aIjI1h8a1MFQHEMB1u-XTW-66XcMeFxIjwceD4RBn1hoUrOkN~sNS42U9MKG6iw7-o19PEZQG9hb7NTV8zGmJeZLa4g4twfTFF8BCqiVBp2CsNPWhWrMrh50E3AVdXq6TIh0sUcj20oGhTK1LUBslY0OFOJtw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":2526,"name":"Polymer Chemistry","url":"https://www.academia.edu/Documents/in/Polymer_Chemistry"},{"id":3408,"name":"Green Chemistry","url":"https://www.academia.edu/Documents/in/Green_Chemistry"},{"id":5596,"name":"Solid Oxide Fuel Cells","url":"https://www.academia.edu/Documents/in/Solid_Oxide_Fuel_Cells"},{"id":16216,"name":"Lanthanide","url":"https://www.academia.edu/Documents/in/Lanthanide"},{"id":57491,"name":"Boron Nitride","url":"https://www.academia.edu/Documents/in/Boron_Nitride"},{"id":58128,"name":"Ceramics","url":"https://www.academia.edu/Documents/in/Ceramics"},{"id":72807,"name":"Natural rubber","url":"https://www.academia.edu/Documents/in/Natural_rubber"},{"id":151442,"name":"Nano Materials","url":"https://www.academia.edu/Documents/in/Nano_Materials"},{"id":391257,"name":"Bismuth Oxide","url":"https://www.academia.edu/Documents/in/Bismuth_Oxide"},{"id":969707,"name":"Ceramics Composites","url":"https://www.academia.edu/Documents/in/Ceramics_Composites"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2016100"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2016100/THE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCONIUM_OXIDE_CERAMIC_PRODUCTION_AT_NANO_DIMENSIONS_USING_YTTRIUM_ACETATE_OR_NITRATE"><img alt="Research paper thumbnail of THE METHOD OF PARTIALLY STABILIZED ZIRCONIUM OXIDE CERAMIC PRODUCTION AT NANO DIMENSIONS USING YTTRIUM ACETATE OR NITRATE " class="work-thumbnail" src="https://attachments.academia-assets.com/29751534/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2016100/THE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCONIUM_OXIDE_CERAMIC_PRODUCTION_AT_NANO_DIMENSIONS_USING_YTTRIUM_ACETATE_OR_NITRATE">THE METHOD OF PARTIALLY STABILIZED ZIRCONIUM OXIDE CERAMIC PRODUCTION AT NANO DIMENSIONS USING YTTRIUM ACETATE OR NITRATE </a></div><div class="wp-workCard_item"><span>Patent No: TR 2009/06608 (Patent veriliş tarihi: 21.09.2012)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">This patent is the production method of zirconium oxide or partially stabilized zirconium oxide m...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">This patent is the production method of zirconium oxide or partially stabilized zirconium oxide material at nano dimensions. Other polymers such as PEG which is called polyethylene glycol, PEO which is called polyethylene oxide, PVAc which is called polyvinyl acetate, PVP which is called polyvinyl pyrrolidone and/or PVA which is called polyvinyl alcohol are used individually or as dual or triple mixtures namely as hybrid copolymers. Zirconium acetate can be used as a source of zirconium and yttrium acetate or nitrate as a source of yttrium can be used in the patent. <br />Boron oxide additive is available in the patent and boric acid is used as a source of boron if required. <br /> The electro-spinned nano-fibers are calcined preferably at 800 oC in preferably an air environment and then the material is transformed into a pellet by being processed in grinders.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="7d2bf8db93e75997c946ced7ff1329ba" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751534,&quot;asset_id&quot;:2016100,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751534/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2016100"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2016100"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2016100; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2016100]").text(description); $(".js-view-count[data-work-id=2016100]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2016100; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2016100']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2016100, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "7d2bf8db93e75997c946ced7ff1329ba" } } $('.js-work-strip[data-work-id=2016100]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2016100,"title":"THE METHOD OF PARTIALLY STABILIZED ZIRCONIUM OXIDE CERAMIC PRODUCTION AT NANO DIMENSIONS USING YTTRIUM ACETATE OR NITRATE ","translated_title":"","metadata":{"abstract":"This patent is the production method of zirconium oxide or partially stabilized zirconium oxide material at nano dimensions. Other polymers such as PEG which is called polyethylene glycol, PEO which is called polyethylene oxide, PVAc which is called polyvinyl acetate, PVP which is called polyvinyl pyrrolidone and/or PVA which is called polyvinyl alcohol are used individually or as dual or triple mixtures namely as hybrid copolymers. Zirconium acetate can be used as a source of zirconium and yttrium acetate or nitrate as a source of yttrium can be used in the patent.\r\nBoron oxide additive is available in the patent and boric acid is used as a source of boron if required.\r\n\tThe electro-spinned nano-fibers are calcined preferably at 800 oC in preferably an air environment and then the material is transformed into a pellet by being processed in grinders.\r\n","ai_title_tag":"Nano-Dimension Zirconium Oxide Production via Yttrium Additives","publication_name":"Patent No: TR 2009/06608 (Patent veriliş tarihi: 21.09.2012)"},"translated_abstract":"This patent is the production method of zirconium oxide or partially stabilized zirconium oxide material at nano dimensions. 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Other polymers such as PEG which is called polyethylene glycol, PEO which is called polyethylene oxide, PVAc which is called polyvinyl acetate, PVP which is called polyvinyl pyrrolidone and/or PVA which is called polyvinyl alcohol are used individually or as dual or triple mixtures namely as hybrid copolymers. Zirconium acetate can be used as a source of zirconium and yttrium acetate or nitrate as a source of yttrium can be used in the patent.\r\nBoron oxide additive is available in the patent and boric acid is used as a source of boron if required.\r\n\tThe electro-spinned nano-fibers are calcined preferably at 800 oC in preferably an air environment and then the material is transformed into a pellet by being processed in grinders.\r\n","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":29751534,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751534/thumbnails/1.jpg","file_name":"Poster_zirconia_son.pdf","download_url":"https://www.academia.edu/attachments/29751534/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"THE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCO.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751534/Poster_zirconia_son-libre.pdf?1390877994=\u0026response-content-disposition=attachment%3B+filename%3DTHE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCO.pdf\u0026Expires=1733756526\u0026Signature=FIEFPDWrInbz8z3jMiOYpR7GSqmNZC1HQtdct5-lfpBBYltzzvzrckvbsRPftb4OrXl-x6Gd3mg6~UEbtDccnR6w2qF3K-pXlXaPgUf4IctbHSCyEUG3FL19UZHdFZjugzrz~4yG-KugxQx9J5~sKH0la0ad9rzr0g2HtryAXUEWDlKs57c3XTOIUaYsdwAPaaoJSToPWs1hf0GAHa2h-DynBvSLXYr8o4ePoWWdWjn~Fw-3EWMMoMpmethpRqRaQlhgfrrcaPXdQKipW5IQKdbByjat5U6xyscmClJbSCyH5dYIFcUZ7InusiN427v-oWJsggU6lXuurieNdmOzrg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":29492586,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29492586/thumbnails/1.jpg","file_name":"06608.pdf","download_url":"https://www.academia.edu/attachments/29492586/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"THE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCO.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29492586/06608-libre.pdf?1390876630=\u0026response-content-disposition=attachment%3B+filename%3DTHE_METHOD_OF_PARTIALLY_STABILIZED_ZIRCO.pdf\u0026Expires=1733756526\u0026Signature=DCL~nfGojMHi6aJMSs8liu7x7z5asR15tEN1oJU-r3FM699LQ2IS9BpBJs1z9Coi5boYB66oSSs7e2Fq-8zjno~Vd2sh6xgQWuERzJoA9SpISzhe8RqtCcg1P7AezNwSJ5N9T-bZS-BU-smRfPtS6Evk~4h-kpz-MeaiG0B1R-5tleao4KE-kMDscqPT6lMgbDXyzFqI2NZj~a1lGL~xvSszD7Rcn8KWDDESmisdaCJjqIf7rcerv-BrHtg~fgyz~q15ZCTbOjSujd~6-moahZpvfz5Nai5~giq35s7CL4hBqWCToXf-OZXyNQEnK7Qd~CJ5mus3BRbdSiEcGikiSA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2016093"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2016093/ELEKTRO_E%C4%9E%C4%B0RME_TEKN%C4%B0%C4%9E%C4%B0YLE_N%C4%B0KEL_VE_BOR_KATKILI_TERMOELEKTR%C4%B0K_SODYUM_KOBALT_OKS%C4%B0T_NANO_KOMPOZ%C4%B0T_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0_ve_%C3%9CRET%C4%B0M%C4%B0"><img alt="Research paper thumbnail of ELEKTRO-EĞİRME TEKNİĞİYLE NİKEL VE BOR KATKILI TERMOELEKTRİK SODYUM KOBALT OKSİT NANO KOMPOZİT ÜRETİM YÖNTEMİ ve ÜRETİMİ " class="work-thumbnail" src="https://attachments.academia-assets.com/29751579/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2016093/ELEKTRO_E%C4%9E%C4%B0RME_TEKN%C4%B0%C4%9E%C4%B0YLE_N%C4%B0KEL_VE_BOR_KATKILI_TERMOELEKTR%C4%B0K_SODYUM_KOBALT_OKS%C4%B0T_NANO_KOMPOZ%C4%B0T_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0_ve_%C3%9CRET%C4%B0M%C4%B0">ELEKTRO-EĞİRME TEKNİĞİYLE NİKEL VE BOR KATKILI TERMOELEKTRİK SODYUM KOBALT OKSİT NANO KOMPOZİT ÜRETİM YÖNTEMİ ve ÜRETİMİ </a></div><div class="wp-workCard_item"><span>Patent No: TR 2010/07672 (İnceleme aşamasında)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu patent elektro-eğirme tekniği kullanarak tercihen nikel katkılı sodyum kobalt oksit üretim yön...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu patent elektro-eğirme tekniği kullanarak tercihen nikel katkılı sodyum kobalt oksit üretim yöntemi ve üretimidir. Elektro-eğrilecek polimer malzemesi olarak tercihen polivinil alkol olarak adlandırılan PVA, poliakrilo nitril olarak adlandırılan PAN, polivinil asetat olarak adlandırılan PVAc gibi diğer polimerler tek tek ya da hibrit kopolimer olarak yani ikili ya da üçlü karışımlar olarak da kullanılmaktadır. <br />Sodyum kaynağı olarak tercihen sodyum asetat istenirse sodyum nitrat, kobalt kaynağı olarak tercihen kobalt asetat istenirse kobalt nitrat, nikel kaynağı olarak tercihen nikel asetat istenirse nikel nitrat buluşta kullanılabilmektedir. <br />İstenirse bor oksit katkısı da patentte mümkün olup bor kaynağı olarak da tercihen borik asit kullanılmaktadır. <br />Elektro-eğrilmiş nano-lifler tercihen 1000 oC’de tercihen hava ortamında kalsine edilmekte, elde edilen seramik malzemedeki karbonun ortamdan tam olarak uzaklaştırılamaması ve seramik malzemenin istenilen düzeyde saf olmaması durumunda istenirse kalsine edilmiş ürün tercihen aynı sıcaklıkta tercihen hava ortamında tekrar ısıl işlemden geçirilirmektedir. Daha sonra malzeme istenirse öğütücülerden geçirilerek tercihen pelet haline dönüştürülmektedir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a5d25619db53250243afe14ee2e06730" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751579,&quot;asset_id&quot;:2016093,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751579/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2016093"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2016093"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2016093; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2016093]").text(description); $(".js-view-count[data-work-id=2016093]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2016093; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2016093']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2016093, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "a5d25619db53250243afe14ee2e06730" } } $('.js-work-strip[data-work-id=2016093]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2016093,"title":"ELEKTRO-EĞİRME TEKNİĞİYLE NİKEL VE BOR KATKILI TERMOELEKTRİK SODYUM KOBALT OKSİT NANO KOMPOZİT ÜRETİM YÖNTEMİ ve ÜRETİMİ ","translated_title":"","metadata":{"abstract":"Bu patent elektro-eğirme tekniği kullanarak tercihen nikel katkılı sodyum kobalt oksit üretim yöntemi ve üretimidir. 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Daha sonra malzeme istenirse öğütücülerden geçirilerek tercihen pelet haline dönüştürülmektedir. \r\n","publication_name":"Patent No: TR 2010/07672 (İnceleme aşamasında)"},"translated_abstract":"Bu patent elektro-eğirme tekniği kullanarak tercihen nikel katkılı sodyum kobalt oksit üretim yöntemi ve üretimidir. 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Daha sonra malzeme istenirse öğütücülerden geçirilerek tercihen pelet haline dönüştürülmektedir. \r\n","internal_url":"https://www.academia.edu/2016093/ELEKTRO_E%C4%9E%C4%B0RME_TEKN%C4%B0%C4%9E%C4%B0YLE_N%C4%B0KEL_VE_BOR_KATKILI_TERMOELEKTR%C4%B0K_SODYUM_KOBALT_OKS%C4%B0T_NANO_KOMPOZ%C4%B0T_%C3%9CRET%C4%B0M_Y%C3%96NTEM%C4%B0_ve_%C3%9CRET%C4%B0M%C4%B0","translated_internal_url":"","created_at":"2012-10-10T19:30:15.995-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[{"id":29751579,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751579/thumbnails/1.jpg","file_name":"termoelektrik_malzeme_uretimi_(1).pdf","download_url":"https://www.academia.edu/attachments/29751579/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"ELEKTRO_EGIRME_TEKNIGIYLE_NIKEL_VE_BOR_K.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751579/termoelektrik_malzeme_uretimi_%281%29-libre.pdf?1390878005=\u0026response-content-disposition=attachment%3B+filename%3DELEKTRO_EGIRME_TEKNIGIYLE_NIKEL_VE_BOR_K.pdf\u0026Expires=1733756526\u0026Signature=IvR4fNVw~sL3-OpZrNqk9mQ6eLiw0UUJbjoLH9bhhF4yFJ7u7b515nb8SfgJhuoWsVVJVbNKg74eyKGN1LKjf2BGd~Mwa8lGG2GNq2qKIlTXgJIWvcgVSQAGgYCo5b3460HA93L8UBi8L37viCunWLi~HEU-wUeFV~1IwfYMHXBe1wv6YsuVHz0trUJsORQUTLqtIrgjH6zCfcdisz4BurRhp7Q3GcZYa9HswmZByrJ89DG2VlBPsFptBr6oOfTyuM9xN5ZHxWlabjKSylall8FV~CJz6mpn1eepxsuvmN8ZsuqdXdlK34ECSlewKeruPkvBSIHVi3sX2iDkfUAV1A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"ELEKTRO_EĞİRME_TEKNİĞİYLE_NİKEL_VE_BOR_KATKILI_TERMOELEKTRİK_SODYUM_KOBALT_OKSİT_NANO_KOMPOZİT_ÜRETİM_YÖNTEMİ_ve_ÜRETİMİ","translated_slug":"","page_count":1,"language":"tr","content_type":"Work","summary":"Bu patent elektro-eğirme tekniği kullanarak tercihen nikel katkılı sodyum kobalt oksit üretim yöntemi ve üretimidir. Elektro-eğrilecek polimer malzemesi olarak tercihen polivinil alkol olarak adlandırılan PVA, poliakrilo nitril olarak adlandırılan PAN, polivinil asetat olarak adlandırılan PVAc gibi diğer polimerler tek tek ya da hibrit kopolimer olarak yani ikili ya da üçlü karışımlar olarak da kullanılmaktadır.\r\nSodyum kaynağı olarak tercihen sodyum asetat istenirse sodyum nitrat, kobalt kaynağı olarak tercihen kobalt asetat istenirse kobalt nitrat, nikel kaynağı olarak tercihen nikel asetat istenirse nikel nitrat buluşta kullanılabilmektedir.\r\nİstenirse bor oksit katkısı da patentte mümkün olup bor kaynağı olarak da tercihen borik asit kullanılmaktadır.\r\nElektro-eğrilmiş nano-lifler tercihen 1000 oC’de tercihen hava ortamında kalsine edilmekte, elde edilen seramik malzemedeki karbonun ortamdan tam olarak uzaklaştırılamaması ve seramik malzemenin istenilen düzeyde saf olmaması durumunda istenirse kalsine edilmiş ürün tercihen aynı sıcaklıkta tercihen hava ortamında tekrar ısıl işlemden geçirilirmektedir. Daha sonra malzeme istenirse öğütücülerden geçirilerek tercihen pelet haline dönüştürülmektedir. \r\n","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[{"id":29751579,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751579/thumbnails/1.jpg","file_name":"termoelektrik_malzeme_uretimi_(1).pdf","download_url":"https://www.academia.edu/attachments/29751579/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"ELEKTRO_EGIRME_TEKNIGIYLE_NIKEL_VE_BOR_K.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751579/termoelektrik_malzeme_uretimi_%281%29-libre.pdf?1390878005=\u0026response-content-disposition=attachment%3B+filename%3DELEKTRO_EGIRME_TEKNIGIYLE_NIKEL_VE_BOR_K.pdf\u0026Expires=1733756526\u0026Signature=IvR4fNVw~sL3-OpZrNqk9mQ6eLiw0UUJbjoLH9bhhF4yFJ7u7b515nb8SfgJhuoWsVVJVbNKg74eyKGN1LKjf2BGd~Mwa8lGG2GNq2qKIlTXgJIWvcgVSQAGgYCo5b3460HA93L8UBi8L37viCunWLi~HEU-wUeFV~1IwfYMHXBe1wv6YsuVHz0trUJsORQUTLqtIrgjH6zCfcdisz4BurRhp7Q3GcZYa9HswmZByrJ89DG2VlBPsFptBr6oOfTyuM9xN5ZHxWlabjKSylall8FV~CJz6mpn1eepxsuvmN8ZsuqdXdlK34ECSlewKeruPkvBSIHVi3sX2iDkfUAV1A__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2016089"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/2016089/KAPARI_B%C4%B0TK%C4%B0S%C4%B0N%C4%B0N_YAPRA%C4%9EIYLA_VEYA_YAPRAKTAK%C4%B0_ETK%C4%B0N_MADDELER%C4%B0N_ELDES%C4%B0_SONUCUNDA_V%C4%B0T%C4%B0L%C4%B0GO_HASTALI%C4%9EININ_TEDAV%C4%B0S%C4%B0"><img alt="Research paper thumbnail of KAPARI BİTKİSİNİN YAPRAĞIYLA VEYA YAPRAKTAKİ ETKİN MADDELERİN ELDESİ SONUCUNDA VİTİLİGO HASTALIĞININ TEDAVİSİ" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/2016089/KAPARI_B%C4%B0TK%C4%B0S%C4%B0N%C4%B0N_YAPRA%C4%9EIYLA_VEYA_YAPRAKTAK%C4%B0_ETK%C4%B0N_MADDELER%C4%B0N_ELDES%C4%B0_SONUCUNDA_V%C4%B0T%C4%B0L%C4%B0GO_HASTALI%C4%9EININ_TEDAV%C4%B0S%C4%B0">KAPARI BİTKİSİNİN YAPRAĞIYLA VEYA YAPRAKTAKİ ETKİN MADDELERİN ELDESİ SONUCUNDA VİTİLİGO HASTALIĞININ TEDAVİSİ</a></div><div class="wp-workCard_item"><span>Patent No: TR 2009/04021 (İncelemeli patent)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Bu buluş Vitiligo olarak adlandırılan ve deriyi boyayan madde olan pigmentlerin kaybı nedeniyle, ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Bu buluş Vitiligo olarak adlandırılan ve deriyi boyayan madde olan pigmentlerin kaybı nedeniyle, cildin beyazlaşması ile seyreden hastalığın, capparis spinosa bitkisinin yaprağındaki özsuyu ile tedavisini içermektedir. Kapari bitkisinin yanı sıra yaprak özsuyununun etken maddelerinin diğer bitkilerden elde edilmesi yada organik olarak sentezlenerek direk olarak yada gliserin, vazelin gibi krem yapıcılarla krem haline getirilerek yada jel haline getirilerek sürülmesi buluşun kapsamı içersindedir.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2016089"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2016089"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2016089; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2016089]").text(description); $(".js-view-count[data-work-id=2016089]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2016089; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2016089']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2016089, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=2016089]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2016089,"title":"KAPARI BİTKİSİNİN YAPRAĞIYLA VEYA YAPRAKTAKİ ETKİN MADDELERİN ELDESİ SONUCUNDA VİTİLİGO HASTALIĞININ TEDAVİSİ","translated_title":"","metadata":{"abstract":"Bu buluş Vitiligo olarak adlandırılan ve deriyi boyayan madde olan pigmentlerin kaybı nedeniyle, cildin beyazlaşması ile seyreden hastalığın, capparis spinosa bitkisinin yaprağındaki özsuyu ile tedavisini içermektedir. Kapari bitkisinin yanı sıra yaprak özsuyununun etken maddelerinin diğer bitkilerden elde edilmesi yada organik olarak sentezlenerek direk olarak yada gliserin, vazelin gibi krem yapıcılarla krem haline getirilerek yada jel haline getirilerek sürülmesi buluşun kapsamı içersindedir.","more_info":"Patent başvurum için Rusya Patent Ofisinin incelemesi tamamlanmış ve İncelemeli patent verilmesine ilişkin koşulları engelleyen bir durum olmadığı belirtilmiş ve Türk patent Enstitüsü (TPE) tarafından başvuruya İncelemeli Patent belgesi verilmesine karar verilmiştir.","publication_name":"Patent No: TR 2009/04021 (İncelemeli patent)"},"translated_abstract":"Bu buluş Vitiligo olarak adlandırılan ve deriyi boyayan madde olan pigmentlerin kaybı nedeniyle, cildin beyazlaşması ile seyreden hastalığın, capparis spinosa bitkisinin yaprağındaki özsuyu ile tedavisini içermektedir. Kapari bitkisinin yanı sıra yaprak özsuyununun etken maddelerinin diğer bitkilerden elde edilmesi yada organik olarak sentezlenerek direk olarak yada gliserin, vazelin gibi krem yapıcılarla krem haline getirilerek yada jel haline getirilerek sürülmesi buluşun kapsamı içersindedir.","internal_url":"https://www.academia.edu/2016089/KAPARI_B%C4%B0TK%C4%B0S%C4%B0N%C4%B0N_YAPRA%C4%9EIYLA_VEYA_YAPRAKTAK%C4%B0_ETK%C4%B0N_MADDELER%C4%B0N_ELDES%C4%B0_SONUCUNDA_V%C4%B0T%C4%B0L%C4%B0GO_HASTALI%C4%9EININ_TEDAV%C4%B0S%C4%B0","translated_internal_url":"","created_at":"2012-10-10T19:26:55.424-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[],"slug":"KAPARI_BİTKİSİNİN_YAPRAĞIYLA_VEYA_YAPRAKTAKİ_ETKİN_MADDELERİN_ELDESİ_SONUCUNDA_VİTİLİGO_HASTALIĞININ_TEDAVİSİ","translated_slug":"","page_count":null,"language":"tr","content_type":"Work","summary":"Bu buluş Vitiligo olarak adlandırılan ve deriyi boyayan madde olan pigmentlerin kaybı nedeniyle, cildin beyazlaşması ile seyreden hastalığın, capparis spinosa bitkisinin yaprağındaki özsuyu ile tedavisini içermektedir. Kapari bitkisinin yanı sıra yaprak özsuyununun etken maddelerinin diğer bitkilerden elde edilmesi yada organik olarak sentezlenerek direk olarak yada gliserin, vazelin gibi krem yapıcılarla krem haline getirilerek yada jel haline getirilerek sürülmesi buluşun kapsamı içersindedir.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="2016087"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/2016087/PREPARATION_OF_ANTIMICROBIAL_NANO_FIBER_WOUND_DRESSING_MATERIAL_USING_PVA_PAA_POLYMERS"><img alt="Research paper thumbnail of PREPARATION OF ANTIMICROBIAL NANO FIBER WOUND DRESSING MATERIAL USING PVA/PAA POLYMERS " class="work-thumbnail" src="https://attachments.academia-assets.com/29751859/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/2016087/PREPARATION_OF_ANTIMICROBIAL_NANO_FIBER_WOUND_DRESSING_MATERIAL_USING_PVA_PAA_POLYMERS">PREPARATION OF ANTIMICROBIAL NANO FIBER WOUND DRESSING MATERIAL USING PVA/PAA POLYMERS </a></div><div class="wp-workCard_item"><span>Patent No: TR 2009/03464 (Patent veriliş tarihi: 21.09.2012)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The innovation involves the preparation of antimicrobial nano fiber wound dressing material from ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The innovation involves the preparation of antimicrobial nano fiber wound dressing material from PVA/PAA hybrid polymer by the addition of&nbsp; anti microbial agents such as PVP or povidon iodine and/or chlorhexidine solution . The nano fibers were obtained with the use electrospinning technique . Electrospinning technique enables the preparation of fibers with a very big surface area to volume ratios. This makes it possible to adjust the pore sizes .The resulting nano fibers are dried by the method indicated in this patent such as using vacuum ovens and sterilization of the resultant fibers by one of the commercial method mentioned in this patent such as irradiation or chemical techniques&nbsp; .</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9a5df18cc5ae87878e73448d4c97dc14" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751859,&quot;asset_id&quot;:2016087,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751859/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2016087"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2016087"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2016087; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2016087]").text(description); $(".js-view-count[data-work-id=2016087]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2016087; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2016087']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2016087, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "9a5df18cc5ae87878e73448d4c97dc14" } } $('.js-work-strip[data-work-id=2016087]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2016087,"title":"PREPARATION OF ANTIMICROBIAL NANO FIBER WOUND DRESSING MATERIAL USING PVA/PAA POLYMERS ","translated_title":"","metadata":{"abstract":"The innovation involves the preparation of antimicrobial nano fiber wound dressing material from PVA/PAA hybrid polymer by the addition of anti microbial agents such as PVP or povidon iodine and/or chlorhexidine solution . The nano fibers were obtained with the use electrospinning technique . Electrospinning technique enables the preparation of fibers with a very big surface area to volume ratios. This makes it possible to adjust the pore sizes .The resulting nano fibers are dried by the method indicated in this patent such as using vacuum ovens and sterilization of the resultant fibers by one of the commercial method mentioned in this patent such as irradiation or chemical techniques .\r\n","publication_name":"Patent No: TR 2009/03464 (Patent veriliş tarihi: 21.09.2012)"},"translated_abstract":"The innovation involves the preparation of antimicrobial nano fiber wound dressing material from PVA/PAA hybrid polymer by the addition of anti microbial agents such as PVP or povidon iodine and/or chlorhexidine solution . The nano fibers were obtained with the use electrospinning technique . Electrospinning technique enables the preparation of fibers with a very big surface area to volume ratios. 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The cerium source is the cerium acetate . It is added to the hybrid polymer / copolymer solution and converted into nano fibers with electro spinning technique&nbsp; . The nano fibers are subjected to calcinations process&nbsp; under air atmosphere . It may be necessary to prolong the calcination process or add oxygen to the medium in order to remove the residual carbon or carbon derivatives from the structure.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a84a6cba0c59e0bca82cc13eb921f754" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751884,&quot;asset_id&quot;:2015929,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751884/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2015929"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2015929"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2015929; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2015929]").text(description); $(".js-view-count[data-work-id=2015929]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2015929; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2015929']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2015929, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "a84a6cba0c59e0bca82cc13eb921f754" } } $('.js-work-strip[data-work-id=2015929]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2015929,"title":"PRODUCTION OF CERIUM OXIDE WITH ELECTROSPINNING METHOD FOR CANCER THREAPHY","translated_title":"","metadata":{"abstract":"This patent involves the production of nano sized cerium oxide for cancer therapy with the use of electro spinning method using a hybrid polymer solution The hybrid polymer solution to be electro spun can be prepared by the single or the copolymer/hybrid polymer solutions or binary or tertiary mixtures of polymers like PEG, PEO, PVAc, PVP and/or PVA . The cerium source is the cerium acetate . It is added to the hybrid polymer / copolymer solution and converted into nano fibers with electro spinning technique . The nano fibers are subjected to calcinations process under air atmosphere . It may be necessary to prolong the calcination process or add oxygen to the medium in order to remove the residual carbon or carbon derivatives from the structure. \r\n","publication_name":"Patent No: TR 2010/03580 (İnceleme aşamasında)"},"translated_abstract":"This patent involves the production of nano sized cerium oxide for cancer therapy with the use of electro spinning method using a hybrid polymer solution The hybrid polymer solution to be electro spun can be prepared by the single or the copolymer/hybrid polymer solutions or binary or tertiary mixtures of polymers like PEG, PEO, PVAc, PVP and/or PVA . The cerium source is the cerium acetate . 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It may be necessary to prolong the calcination process or add oxygen to the medium in order to remove the residual carbon or carbon derivatives from the structure. \r\n","internal_url":"https://www.academia.edu/2015929/PRODUCTION_OF_CERIUM_OXIDE_WITH_ELECTROSPINNING_METHOD_FOR_CANCER_THREAPHY","translated_internal_url":"","created_at":"2012-10-10T18:47:18.019-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[{"id":29751884,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/29751884/thumbnails/1.jpg","file_name":"Ce_poster_son.pdf","download_url":"https://www.academia.edu/attachments/29751884/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"PRODUCTION_OF_CERIUM_OXIDE_WITH_ELECTROS.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/29751884/Ce_poster_son-libre.pdf?1390878014=\u0026response-content-disposition=attachment%3B+filename%3DPRODUCTION_OF_CERIUM_OXIDE_WITH_ELECTROS.pdf\u0026Expires=1733756526\u0026Signature=cqkQX29yRIQKVjK5~UHwlZF4HBOBCivNXzQnqPkJHOMYNuEj1XzeMJePrDl5jKTKwhWBUi6rjy~SeAPy7sYycxkQnCBza4bWaovBfs48A3g80V-lWRfcD6btMzuYsc7fVf7MQur5hI~C8TdLLEprgAN~EYt5hvveEiItBLbQSknElv-d5LGBpBOcjPVpAKsuLYs6JqL55f50bfikrB-t265iLwqc9TXSNUam6wZ5QfjMtJk63SeBFLsBtxl8IR2413p50jCNWE2mWsQhiqFvWT7D9vRI802iC1JcVdT8MZ0ZSD8oNO~vcA960U6zaCdEXheVKiafOueSB4zX2fPtVA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"PRODUCTION_OF_CERIUM_OXIDE_WITH_ELECTROSPINNING_METHOD_FOR_CANCER_THREAPHY","translated_slug":"","page_count":1,"language":"tr","content_type":"Work","summary":"This patent involves the production of nano sized cerium oxide for cancer therapy with the use of electro spinning method using a hybrid polymer solution The hybrid polymer solution to be electro spun can be prepared by the single or the copolymer/hybrid polymer solutions or binary or tertiary mixtures of polymers like PEG, PEO, PVAc, PVP and/or PVA . 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It enables the coverage of advanced nuclear fuels with boron nitride with the use of ammonia and boron tribromide.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="692b662392581a76e4c90697e79ec389" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:29751897,&quot;asset_id&quot;:2015925,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/29751897/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="2015925"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="2015925"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 2015925; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=2015925]").text(description); $(".js-view-count[data-work-id=2015925]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 2015925; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='2015925']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 2015925, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "692b662392581a76e4c90697e79ec389" } } $('.js-work-strip[data-work-id=2015925]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":2015925,"title":"PREPARATION OF BORON NITRIDE COVERED NUCLEAR FUEL BY THE USE OF BORON TRIBROMIDE ","translated_title":"","metadata":{"abstract":"This innovation related the coverage of preferably pelleted uranium dioxide nuclear fuel containing various amount of combustible poison such as gadolinium oxide with boron nitride. 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Özellikle de yarın..." class="work-thumbnail" src="https://attachments.academia-assets.com/43264401/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/22684495/%C3%87%C3%B6l_tozlar%C4%B1na_dikkat_%C3%96zellikle_de_yar%C4%B1n_">Çöl tozlarına dikkat! Özellikle de yarın...</a></div><div class="wp-workCard_item"><span>Çöl tozlarına dikkat! Özellikle de yarın...</span><span>, Mar 2, 2016</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Gazi Üniversitesi Eğitim Fakültesi Kimya Eğitimi Ana Bilim Dalı Öğretim Üyesi Prof. Dr. İbrahim U...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Gazi Üniversitesi Eğitim Fakültesi Kimya Eğitimi Ana Bilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, sahradan şiddetli rüzgarlarla gelen çöl tozlarının bir haftadır Türkiye üzerinde biriktiğini belirterek &quot;3 Mart&#39;ta yoğunlaşacak toz bulutları, 6 Mart&#39;ta ülkemizi terk edecek&quot; dedi.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="79a83477201a7c96e4dfbe3b1dd2b2d0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:43264401,&quot;asset_id&quot;:22684495,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/43264401/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="22684495"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22684495"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22684495; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22684495]").text(description); $(".js-view-count[data-work-id=22684495]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22684495; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22684495']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 22684495, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "79a83477201a7c96e4dfbe3b1dd2b2d0" } } $('.js-work-strip[data-work-id=22684495]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22684495,"title":"Çöl tozlarına dikkat! 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Benden 5 yaş küçük olan bu çok değerli iş adamımızın yaşasaydı ülkemizin kalkınmasına daha çok katkıları olacaktı. Ancak değerli iş adamlarımızı çevresinden yardım aldıkları diyetisyen vb sağlıkla ilgili danışmanlarının iyi yönlendiremediklerini şimdi Mustafa Koç&#39;un resminden vereceğim örneklerle açıklamak istiyorum. Bir kere gözler ve yüz başta olmak üzere vücudumuz hastalıkların habercisidir. Ben bir insanın yüzüne bakınca hangi hastalıkları olduğunu rahatlıkla anlarım. Bu böyle değerli bir iş adamının çevresindeki diyetisyen vb sağlık danışmanlarının da bilmesi gereken bir özellik olmalıdır. Ancak anlaşılıyor ki maalesef kendisine sağlığını düzeltmesiyle ilgili tedbirlerin alınmasını sağlayacak gerekli bilgiler verilmemiş.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="59b69e9012684bb15e0a39b3213b14d5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:41616994,&quot;asset_id&quot;:20850012,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/41616994/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="20850012"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="20850012"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 20850012; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=20850012]").text(description); $(".js-view-count[data-work-id=20850012]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 20850012; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='20850012']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 20850012, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "59b69e9012684bb15e0a39b3213b14d5" } } $('.js-work-strip[data-work-id=20850012]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":20850012,"title":"HASTALIĞIMIZ YÜZÜMÜZE YAZILMIŞTIR","translated_title":"","metadata":{"abstract":"HASTALIĞIMIZ YÜZÜMÜZE YAZILMIŞTIR\nKardeşlerim, Ülkemizin en değerli iş adamlarından Mustafa Koç'u kaybetmenin derin üzüntüsü yaşamaktayım. Benden 5 yaş küçük olan bu çok değerli iş adamımızın yaşasaydı ülkemizin kalkınmasına daha çok katkıları olacaktı. Ancak değerli iş adamlarımızı çevresinden yardım aldıkları diyetisyen vb sağlıkla ilgili danışmanlarının iyi yönlendiremediklerini şimdi Mustafa Koç'un resminden vereceğim örneklerle açıklamak istiyorum. Bir kere gözler ve yüz başta olmak üzere vücudumuz hastalıkların habercisidir. Ben bir insanın yüzüne bakınca hangi hastalıkları olduğunu rahatlıkla anlarım. Bu böyle değerli bir iş adamının çevresindeki diyetisyen vb sağlık danışmanlarının da bilmesi gereken bir özellik olmalıdır. Ancak anlaşılıyor ki maalesef kendisine sağlığını düzeltmesiyle ilgili tedbirlerin alınmasını sağlayacak gerekli bilgiler verilmemiş."},"translated_abstract":"HASTALIĞIMIZ YÜZÜMÜZE YAZILMIŞTIR\nKardeşlerim, Ülkemizin en değerli iş adamlarından Mustafa Koç'u kaybetmenin derin üzüntüsü yaşamaktayım. Benden 5 yaş küçük olan bu çok değerli iş adamımızın yaşasaydı ülkemizin kalkınmasına daha çok katkıları olacaktı. Ancak değerli iş adamlarımızı çevresinden yardım aldıkları diyetisyen vb sağlıkla ilgili danışmanlarının iyi yönlendiremediklerini şimdi Mustafa Koç'un resminden vereceğim örneklerle açıklamak istiyorum. Bir kere gözler ve yüz başta olmak üzere vücudumuz hastalıkların habercisidir. Ben bir insanın yüzüne bakınca hangi hastalıkları olduğunu rahatlıkla anlarım. Bu böyle değerli bir iş adamının çevresindeki diyetisyen vb sağlık danışmanlarının da bilmesi gereken bir özellik olmalıdır. 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Benden 5 yaş küçük olan bu çok değerli iş adamımızın yaşasaydı ülkemizin kalkınmasına daha çok katkıları olacaktı. Ancak değerli iş adamlarımızı çevresinden yardım aldıkları diyetisyen vb sağlıkla ilgili danışmanlarının iyi yönlendiremediklerini şimdi Mustafa Koç'un resminden vereceğim örneklerle açıklamak istiyorum. Bir kere gözler ve yüz başta olmak üzere vücudumuz hastalıkların habercisidir. Ben bir insanın yüzüne bakınca hangi hastalıkları olduğunu rahatlıkla anlarım. Bu böyle değerli bir iş adamının çevresindeki diyetisyen vb sağlık danışmanlarının da bilmesi gereken bir özellik olmalıdır. 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Prof. Uslu, söyleşide kısırlaştırma projesi, kısırlaştırma projesinin bir aracı olan aşılar, kısırlaştırma ve nüfus azaltmanın bir yöntemi olan GDO’lu gıdalara ilişkin önemli bilgiler verdi.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="68190014c2305c5528ed47589245afa4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:41549052,&quot;asset_id&quot;:20764359,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/41549052/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="20764359"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="20764359"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 20764359; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=20764359]").text(description); $(".js-view-count[data-work-id=20764359]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 20764359; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='20764359']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 20764359, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "68190014c2305c5528ed47589245afa4" } } $('.js-work-strip[data-work-id=20764359]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":20764359,"title":"Dünya nüfusu kısırlaştırılıyor","translated_title":"","metadata":{"abstract":"Sahipkıran Stratejik Araştırmalar Merkezi’nin (SASAM) düzenlediği “GDO’lu Besinler, Gıda Güvenliği ve Kısırlık” konulu söyleşiye konuk olan Nano Bilim, Nano Teknoloji ve Nano Tıp Derneği (NANO) Yönetim Kurulu Başkanı ve Gazi Üniversitesi Öğretim Üyesi Prof. Dr. İbrahim Uslu çarpıcı açıklamalarda bulundu. Prof. Uslu, söyleşide kısırlaştırma projesi, kısırlaştırma projesinin bir aracı olan aşılar, kısırlaştırma ve nüfus azaltmanın bir yöntemi olan GDO’lu gıdalara ilişkin önemli bilgiler verdi.","more_info":"Dünya nüfusu kısırlaştırılıyor Nano Bilim, Nano Teknoloji ve Nano Tıp Derneği Yönetim Kurulu Başkanı Prof. Dr. İbrahim Uslu tartışma yaratacak açıklamalarda bulundu.","publisher":"haber7.com","publication_date":{"day":25,"month":1,"year":2016,"errors":{}}},"translated_abstract":"Sahipkıran Stratejik Araştırmalar Merkezi’nin (SASAM) düzenlediği “GDO’lu Besinler, Gıda Güvenliği ve Kısırlık” konulu söyleşiye konuk olan Nano Bilim, Nano Teknoloji ve Nano Tıp Derneği (NANO) Yönetim Kurulu Başkanı ve Gazi Üniversitesi Öğretim Üyesi Prof. Dr. İbrahim Uslu çarpıcı açıklamalarda bulundu. 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data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, kaparinin dünyanın en önde gelen, vücuda zarar veren ögeleri etkisiz hale getiren flavonoid içeren gıda olduğunu belirtti.<br />Genellikle Ege ve Akdeniz sahillerinde yetişen kaparinin, içerdiği flavonoid dolayısıyla hücrelere zarar vererek çeşitli hastalıklara yol açan maddeleri etkisiz hale getirdiği bildirildi.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="677102d42f2667cc32b3e80b335e4f5d" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" 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wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/20655402/Mucizenin_ad%C4%B1_Defne">Mucizenin adı:Defne</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Kimya mühendisi “nükleer bilimler” doçenti olan Prof.Dr. İbrahim Uslu ile projelerini konuştuk. D...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Kimya mühendisi “nükleer bilimler” doçenti olan Prof.Dr. İbrahim Uslu ile projelerini konuştuk. Defnenin mucizesinden ve güneş enerjisinin faydalarından bahseden Prof.Dr. Uslu, başarının sırrının hedef koymak olduğunu anlattı</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="bc7132c06a85324854b83ac811f4bc9f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:41488449,&quot;asset_id&quot;:20655402,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/41488449/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="20655402"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="20655402"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 20655402; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=20655402]").text(description); $(".js-view-count[data-work-id=20655402]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 20655402; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='20655402']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 20655402, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "bc7132c06a85324854b83ac811f4bc9f" } } $('.js-work-strip[data-work-id=20655402]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":20655402,"title":"Mucizenin adı:Defne","translated_title":"","metadata":{"abstract":"Kimya mühendisi “nükleer bilimler” doçenti olan Prof.Dr. İbrahim Uslu ile projelerini konuştuk. 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Ultrasonun jinekologların stetoskobu haline geldiğini belirten Prof. Cansun Demir, hamilelerde ultrasona kısıtlama getirilmesi gerektiğini söyledi." class="work-thumbnail" src="https://attachments.academia-assets.com/36195680/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/10068499/Fare_deneyleri_hamilelikte_ultrasonun_uzun_s%C3%BCre_kullan%C4%B1m%C4%B1n%C4%B1n_kalbe_zararl%C4%B1_olabilece%C4%9Fini_g%C3%B6steriyor_Ultrasonun_jinekologlar%C4%B1n_stetoskobu_haline_geldi%C4%9Fini_belirten_Prof_Cansun_Demir_hamilelerde_ultrasona_k%C4%B1s%C4%B1tlama_getirilmesi_gerekti%C4%9Fini_s%C3%B6yledi">Fare deneyleri, hamilelikte ultrasonun uzun süre kullanımının kalbe zararlı olabileceğini gösteriyor. Ultrasonun jinekologların stetoskobu haline geldiğini belirten Prof. Cansun Demir, hamilelerde ultrasona kısıtlama getirilmesi gerektiğini söyledi.</a></div><div class="wp-workCard_item"><span>NTVMSNBC.com</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Ultrasonun ses dalgası olduğunu ve gebelikteki olumsuz etkileriyle ilgili henüz bilimsel bir kanı...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Ultrasonun ses dalgası olduğunu ve gebelikteki olumsuz etkileriyle ilgili henüz bilimsel bir kanıt bulunmadığını belirten Türk Jinekoloji ve Obstetrik Derneği (TJOD) Genel Sekreteri Prof. Dr. Cansun Demir, ABD başta olmak üzere gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin sınırlı sayıda yapıldığını söyledi. <br /> <br />ABD&#39;de problem olmadığı sürece hamilelere ultrasonla 3 kez bakılıyor. 11-14. haftada ense kalınlığına, 18-22. haftada anatomik gelişime ve gebeliğin son döneminde de bebeğin ters gelip gelmediğine bakıldığını belirten Prof. Demir’e göre, Türkiye&#39;deki hamilelerde ultrason kullanım sıklığı dünya standartlarının üzerinde.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f3e5089baef2758fa72a31c16a18cb01" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{&quot;attachment_id&quot;:36195680,&quot;asset_id&quot;:10068499,&quot;asset_type&quot;:&quot;Work&quot;,&quot;button_location&quot;:&quot;profile&quot;}" href="https://www.academia.edu/attachments/36195680/download_file?st=MTczMzkwMTgzMyw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="10068499"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="10068499"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 10068499; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=10068499]").text(description); $(".js-view-count[data-work-id=10068499]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 10068499; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='10068499']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 10068499, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "f3e5089baef2758fa72a31c16a18cb01" } } $('.js-work-strip[data-work-id=10068499]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":10068499,"title":"Fare deneyleri, hamilelikte ultrasonun uzun süre kullanımının kalbe zararlı olabileceğini gösteriyor. 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$a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="8373929"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/8373929/Ultrason_gibi_kontrollerin_gereksiz_kullan%C4%B1m%C4%B1_yayg%C4%B1n"><img alt="Research paper thumbnail of Ultrason gibi kontrollerin gereksiz kullanımı yaygın" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/8373929/Ultrason_gibi_kontrollerin_gereksiz_kullan%C4%B1m%C4%B1_yayg%C4%B1n">Ultrason gibi kontrollerin gereksiz kullanımı yaygın</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Tıbbi cihazlar gelişip, tıbbi olanaklar genişledikçe, bunların aşırı ve gereksiz kullanımı sorunu...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Tıbbi cihazlar gelişip, tıbbi olanaklar genişledikçe, bunların aşırı ve gereksiz kullanımı sorunu da kendini gösteriyor. Bilindiği gibi, ultrason, röntgen, emar gibi kontrollerin çeşitli yan etkileri nedeniyle ancak gerekli durumlarda yapılması tavsiye ediliyor, aşırı kullanımdan sakınılması gereği sıkça dile getiriliyor.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="8373929"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="8373929"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 8373929; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=8373929]").text(description); $(".js-view-count[data-work-id=8373929]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 8373929; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='8373929']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 8373929, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=8373929]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":8373929,"title":"Ultrason gibi kontrollerin gereksiz kullanımı yaygın","translated_title":"","metadata":{"abstract":"Tıbbi cihazlar gelişip, tıbbi olanaklar genişledikçe, bunların aşırı ve gereksiz kullanımı sorunu da kendini gösteriyor. Bilindiği gibi, ultrason, röntgen, emar gibi kontrollerin çeşitli yan etkileri nedeniyle ancak gerekli durumlarda yapılması tavsiye ediliyor, aşırı kullanımdan sakınılması gereği sıkça dile getiriliyor.","more_info":"Fare deneyleri, hamilelikte ultrasonun uzun süre kullanımının kalbe zararlı olabileceğini gösteriyor. Ultrasonun jinekologların stetoskobu haline geldiğini belirten Prof. Cansun Demir, hamilelerde ultrasona kısıtlama getirilmesi gerektiğini söyledi."},"translated_abstract":"Tıbbi cihazlar gelişip, tıbbi olanaklar genişledikçe, bunların aşırı ve gereksiz kullanımı sorunu da kendini gösteriyor. Bilindiği gibi, ultrason, röntgen, emar gibi kontrollerin çeşitli yan etkileri nedeniyle ancak gerekli durumlarda yapılması tavsiye ediliyor, aşırı kullanımdan sakınılması gereği sıkça dile getiriliyor.","internal_url":"https://www.academia.edu/8373929/Ultrason_gibi_kontrollerin_gereksiz_kullan%C4%B1m%C4%B1_yayg%C4%B1n","translated_internal_url":"","created_at":"2014-09-17T19:26:04.460-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[],"slug":"Ultrason_gibi_kontrollerin_gereksiz_kullanımı_yaygın","translated_slug":"","page_count":null,"language":"tr","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":4270,"name":"Autism Spectrum Disorders","url":"https://www.academia.edu/Documents/in/Autism_Spectrum_Disorders"},{"id":141702,"name":"Fetus Protection","url":"https://www.academia.edu/Documents/in/Fetus_Protection"},{"id":667577,"name":"Otizm","url":"https://www.academia.edu/Documents/in/Otizm"},{"id":1420111,"name":"Otizm Spektrum Bozuklukları","url":"https://www.academia.edu/Documents/in/Otizm_Spektrum_Bozukluklari"},{"id":1558617,"name":"Otistik Bebekler","url":"https://www.academia.edu/Documents/in/Otistik_Bebekler"}],"urls":[{"id":3506129,"url":"http://24haberler.com/saglik/ultrason-kontrolunun-fazlasi-bebege-zararli/"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="8373812"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/8373812/Fay_Hatt%C4%B1_Bodrumu_Etkilemeyecek_Gibi_G%C3%B6r%C3%BCn%C3%BCyor"><img alt="Research paper thumbnail of Fay Hattı Bodrum&#39;u Etkilemeyecek Gibi Görünüyor" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/8373812/Fay_Hatt%C4%B1_Bodrumu_Etkilemeyecek_Gibi_G%C3%B6r%C3%BCn%C3%BCyor">Fay Hattı Bodrum&#39;u Etkilemeyecek Gibi Görünüyor</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrah...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, &quot;Oraklar&#39;dan sonra Karaada&#39;nın hemen arkasından İstanköy&#39;ün yerleşimin pek olmadığı arka taraflarına kayan fay hattı Bodrum&#39;u pek etkilemeyecek gibi görünmektedir&quot; dedi.<br /><br />Uslu, geçmişte Bodrum-İstanköy arasında olan büyük depremlere bakıldığında neredeyse her 96-100 yıl arasında bir büyük deprem olduğunun görüleceğini belirtti. <br />Bodrum Yarımadası&#39;nda iki kırık bulunduğunu aktaran Uslu, iki kırığın tam Karaada&#39;nın olduğu yerde kesiştiğini dile getirdi. <br /><br />Bodrum&#39;un karşısında bulunan özellikle Karaada içindeki sıcak su ve mağaraların jeolojik faaliyetlerin göstergesi olduğunu vurgulayan Uslu, deprem olursa bu noktadan başlayabileceğini anımsattı.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="8373812"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="8373812"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 8373812; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=8373812]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":8373812,"title":"Fay Hattı Bodrum'u Etkilemeyecek Gibi Görünüyor","translated_title":"","metadata":{"abstract":"Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, \"Oraklar'dan sonra Karaada'nın hemen arkasından İstanköy'ün yerleşimin pek olmadığı arka taraflarına kayan fay hattı Bodrum'u pek etkilemeyecek gibi görünmektedir\" dedi.\n\nUslu, geçmişte Bodrum-İstanköy arasında olan büyük depremlere bakıldığında neredeyse her 96-100 yıl arasında bir büyük deprem olduğunun görüleceğini belirtti. \nBodrum Yarımadası'nda iki kırık bulunduğunu aktaran Uslu, iki kırığın tam Karaada'nın olduğu yerde kesiştiğini dile getirdi. \n\nBodrum'un karşısında bulunan özellikle Karaada içindeki sıcak su ve mağaraların jeolojik faaliyetlerin göstergesi olduğunu vurgulayan Uslu, deprem olursa bu noktadan başlayabileceğini anımsattı."},"translated_abstract":"Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, \"Oraklar'dan sonra Karaada'nın hemen arkasından İstanköy'ün yerleşimin pek olmadığı arka taraflarına kayan fay hattı Bodrum'u pek etkilemeyecek gibi görünmektedir\" dedi.\n\nUslu, geçmişte Bodrum-İstanköy arasında olan büyük depremlere bakıldığında neredeyse her 96-100 yıl arasında bir büyük deprem olduğunun görüleceğini belirtti. \nBodrum Yarımadası'nda iki kırık bulunduğunu aktaran Uslu, iki kırığın tam Karaada'nın olduğu yerde kesiştiğini dile getirdi. \n\nBodrum'un karşısında bulunan özellikle Karaada içindeki sıcak su ve mağaraların jeolojik faaliyetlerin göstergesi olduğunu vurgulayan Uslu, deprem olursa bu noktadan başlayabileceğini anımsattı.","internal_url":"https://www.academia.edu/8373812/Fay_Hatt%C4%B1_Bodrumu_Etkilemeyecek_Gibi_G%C3%B6r%C3%BCn%C3%BCyor","translated_internal_url":"","created_at":"2014-09-17T19:18:27.869-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[],"slug":"Fay_Hattı_Bodrumu_Etkilemeyecek_Gibi_Görünüyor","translated_slug":"","page_count":null,"language":"tr","content_type":"Work","summary":"Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, \"Oraklar'dan sonra Karaada'nın hemen arkasından İstanköy'ün yerleşimin pek olmadığı arka taraflarına kayan fay hattı Bodrum'u pek etkilemeyecek gibi görünmektedir\" dedi.\n\nUslu, geçmişte Bodrum-İstanköy arasında olan büyük depremlere bakıldığında neredeyse her 96-100 yıl arasında bir büyük deprem olduğunun görüleceğini belirtti. \nBodrum Yarımadası'nda iki kırık bulunduğunu aktaran Uslu, iki kırığın tam Karaada'nın olduğu yerde kesiştiğini dile getirdi. \n\nBodrum'un karşısında bulunan özellikle Karaada içindeki sıcak su ve mağaraların jeolojik faaliyetlerin göstergesi olduğunu vurgulayan Uslu, deprem olursa bu noktadan başlayabileceğini anımsattı.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":400,"name":"Earth Sciences","url":"https://www.academia.edu/Documents/in/Earth_Sciences"},{"id":2370,"name":"Earthquake Engineering","url":"https://www.academia.edu/Documents/in/Earthquake_Engineering"},{"id":280798,"name":"Deprem","url":"https://www.academia.edu/Documents/in/Deprem"},{"id":444371,"name":"Bodrum","url":"https://www.academia.edu/Documents/in/Bodrum"},{"id":979256,"name":"Deprem Dönüşümü","url":"https://www.academia.edu/Documents/in/Deprem_Donusumu"},{"id":1211947,"name":"İStanköy","url":"https://www.academia.edu/Documents/in/IStankoy"},{"id":1558605,"name":"Cos Island","url":"https://www.academia.edu/Documents/in/Cos_Island"}],"urls":[{"id":3506088,"url":"http://www.haberler.com/bodrum-daki-deprem-6397779-haberi/"},{"id":3506092,"url":"http://www.konhaber.com/yeni/haber-183378-GUNCEL-Bodrumdaki-deprem.html"},{"id":3506094,"url":"http://www.pusulahaber.com.tr/bodrumdaki-deprem-61370h.htm"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="8373664"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/8373664/Ultrasonda_bebe%C4%9Fimin_kula%C4%9F%C4%B1_kep%C3%A7e_mi_diye_bak%C4%B1yorlar"><img alt="Research paper thumbnail of Ultrasonda &quot;bebeğimin kulağı kepçe mi&quot; diye bakıyorlar. " class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/8373664/Ultrasonda_bebe%C4%9Fimin_kula%C4%9F%C4%B1_kep%C3%A7e_mi_diye_bak%C4%B1yorlar">Ultrasonda &quot;bebeğimin kulağı kepçe mi&quot; diye bakıyorlar. </a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Uslu, gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin olumsuz bir durum olmadığı ...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Uslu, gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin olumsuz bir durum olmadığı sürece en fazla üç kez yapıldığını ifade etti. <br /> <br />Söz konusu ülkelerde, 11-14&#39;ncü haftada ense kalınlığına, 18-22&#39;nci haftada anatomik gelişimine, gebeliğin son döneminde de bebeğin ters gelip gelmediğine bakıldığını dile getiren Uslu, Türkiye&#39;deki hamilelerde ultrason kullanım sıklığının dünya standartlarının çok üzerinde olduğuna dikkati çekti. <br /> <br />Türkiye&#39;de hamile, her doktora gittiğinde bebeğe ultrasonla bakıldığını ifade eden Uslu, &quot;Sanki ultrasonun hiç zararı yokmuş gibi bazen dakikalarca, &#39;Bebeğin eli ayağı düzgün mü, bebek kime benziyor, kulağı kepçe mi?&#39; gibi tıbbi olmayan gerekçelerle bakılır oldu ülkemizde&quot; diye konuştu.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="8373664"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="8373664"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 8373664; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=8373664]").text(description); $(".js-view-count[data-work-id=8373664]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 8373664; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='8373664']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 8373664, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=8373664]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":8373664,"title":"Ultrasonda \"bebeğimin kulağı kepçe mi\" diye bakıyorlar. ","translated_title":"","metadata":{"abstract":"Uslu, gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin olumsuz bir durum olmadığı sürece en fazla üç kez yapıldığını ifade etti.\r\n\r\nSöz konusu ülkelerde, 11-14'ncü haftada ense kalınlığına, 18-22'nci haftada anatomik gelişimine, gebeliğin son döneminde de bebeğin ters gelip gelmediğine bakıldığını dile getiren Uslu, Türkiye'deki hamilelerde ultrason kullanım sıklığının dünya standartlarının çok üzerinde olduğuna dikkati çekti.\r\n\r\nTürkiye'de hamile, her doktora gittiğinde bebeğe ultrasonla bakıldığını ifade eden Uslu, \"Sanki ultrasonun hiç zararı yokmuş gibi bazen dakikalarca, 'Bebeğin eli ayağı düzgün mü, bebek kime benziyor, kulağı kepçe mi?' gibi tıbbi olmayan gerekçelerle bakılır oldu ülkemizde\" diye konuştu."},"translated_abstract":"Uslu, gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin olumsuz bir durum olmadığı sürece en fazla üç kez yapıldığını ifade etti.\r\n\r\nSöz konusu ülkelerde, 11-14'ncü haftada ense kalınlığına, 18-22'nci haftada anatomik gelişimine, gebeliğin son döneminde de bebeğin ters gelip gelmediğine bakıldığını dile getiren Uslu, Türkiye'deki hamilelerde ultrason kullanım sıklığının dünya standartlarının çok üzerinde olduğuna dikkati çekti.\r\n\r\nTürkiye'de hamile, her doktora gittiğinde bebeğe ultrasonla bakıldığını ifade eden Uslu, \"Sanki ultrasonun hiç zararı yokmuş gibi bazen dakikalarca, 'Bebeğin eli ayağı düzgün mü, bebek kime benziyor, kulağı kepçe mi?' gibi tıbbi olmayan gerekçelerle bakılır oldu ülkemizde\" diye konuştu.","internal_url":"https://www.academia.edu/8373664/Ultrasonda_bebe%C4%9Fimin_kula%C4%9F%C4%B1_kep%C3%A7e_mi_diye_bak%C4%B1yorlar","translated_internal_url":"","created_at":"2014-09-17T19:11:37.148-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[],"slug":"Ultrasonda_bebeğimin_kulağı_kepçe_mi_diye_bakıyorlar","translated_slug":"","page_count":null,"language":"tr","content_type":"Work","summary":"Uslu, gelişmiş ülkelerde anne karnındaki bebeğin ultrasonla takibinin olumsuz bir durum olmadığı sürece en fazla üç kez yapıldığını ifade etti.\r\n\r\nSöz konusu ülkelerde, 11-14'ncü haftada ense kalınlığına, 18-22'nci haftada anatomik gelişimine, gebeliğin son döneminde de bebeğin ters gelip gelmediğine bakıldığını dile getiren Uslu, Türkiye'deki hamilelerde ultrason kullanım sıklığının dünya standartlarının çok üzerinde olduğuna dikkati çekti.\r\n\r\nTürkiye'de hamile, her doktora gittiğinde bebeğe ultrasonla bakıldığını ifade eden Uslu, \"Sanki ultrasonun hiç zararı yokmuş gibi bazen dakikalarca, 'Bebeğin eli ayağı düzgün mü, bebek kime benziyor, kulağı kepçe mi?' gibi tıbbi olmayan gerekçelerle bakılır oldu ülkemizde\" diye konuştu.","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[{"id":4522,"name":"Ultrasound Imaging","url":"https://www.academia.edu/Documents/in/Ultrasound_Imaging"},{"id":7497,"name":"ULTRASOUND/ACOUSTICS","url":"https://www.academia.edu/Documents/in/ULTRASOUND_ACOUSTICS"},{"id":10269,"name":"Medical Ultrasound Physics","url":"https://www.academia.edu/Documents/in/Medical_Ultrasound_Physics"},{"id":15639,"name":"Ultrasound","url":"https://www.academia.edu/Documents/in/Ultrasound"},{"id":71935,"name":"Doppler Ultrasound","url":"https://www.academia.edu/Documents/in/Doppler_Ultrasound"},{"id":141702,"name":"Fetus Protection","url":"https://www.academia.edu/Documents/in/Fetus_Protection"},{"id":604288,"name":"Ultrasound guided regional anesthesia","url":"https://www.academia.edu/Documents/in/Ultrasound_guided_regional_anesthesia"},{"id":667577,"name":"Otizm","url":"https://www.academia.edu/Documents/in/Otizm"},{"id":770944,"name":"Fetus","url":"https://www.academia.edu/Documents/in/Fetus"},{"id":1420111,"name":"Otizm Spektrum Bozuklukları","url":"https://www.academia.edu/Documents/in/Otizm_Spektrum_Bozukluklari"}],"urls":[{"id":3506017,"url":"http://www.hurriyet.com.tr/kelebek/saglik/27132380.asp"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="8203140"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/8203140/Bu_%C3%BClkede_b%C3%B6yle_doktorlar_var"><img alt="Research paper thumbnail of Bu ülkede böyle doktorlar var" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/8203140/Bu_%C3%BClkede_b%C3%B6yle_doktorlar_var">Bu ülkede böyle doktorlar var</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Kardeşlerim size çok komik bir durum göstermek istiyorum. Ultrasonun zararsız olduğunu http://www...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Kardeşlerim size çok komik bir durum göstermek istiyorum. Ultrasonun zararsız olduğunu <a href="http://www.ntvmsnbc.com/id/25535620/" rel="nofollow">http://www.ntvmsnbc.com/id/25535620/</a> haberinde söyleyen bu doktor bey 23 Mayıs 2011 de yine ultrason kullanımı bebeğin kalbine zarar verir diyor.<br />İşte haberi: <a href="http://www.ntvmsnbc.com/id/25215605/" rel="nofollow">http://www.ntvmsnbc.com/id/25215605/</a><br />Ey doktor kardeşim, 3 senede ultrason zararlı diyen sen, şimdi çıkmışsın ve bu milletin gözünün içine baka baka ultrasonun hiç zararı yoktur diyorsun.<br />Benim sana söyleyecek hiç sözüm yok.<br />Seni yüce Rabbimle baş başa bırakıyorum. seni Allahımla baş başa bırakıyorum.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="8203140"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="8203140"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 8203140; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=8203140]").text(description); $(".js-view-count[data-work-id=8203140]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 8203140; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='8203140']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 8203140, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=8203140]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":8203140,"title":"Bu ülkede böyle doktorlar var","translated_title":"","metadata":{"abstract":"Kardeşlerim size çok komik bir durum göstermek istiyorum. Ultrasonun zararsız olduğunu http://www.ntvmsnbc.com/id/25535620/ haberinde söyleyen bu doktor bey 23 Mayıs 2011 de yine ultrason kullanımı bebeğin kalbine zarar verir diyor.\nİşte haberi: http://www.ntvmsnbc.com/id/25215605/\nEy doktor kardeşim, 3 senede ultrason zararlı diyen sen, şimdi çıkmışsın ve bu milletin gözünün içine baka baka ultrasonun hiç zararı yoktur diyorsun.\nBenim sana söyleyecek hiç sözüm yok.\nSeni yüce Rabbimle baş başa bırakıyorum. seni Allahımla baş başa bırakıyorum."},"translated_abstract":"Kardeşlerim size çok komik bir durum göstermek istiyorum. Ultrasonun zararsız olduğunu http://www.ntvmsnbc.com/id/25535620/ haberinde söyleyen bu doktor bey 23 Mayıs 2011 de yine ultrason kullanımı bebeğin kalbine zarar verir diyor.\nİşte haberi: http://www.ntvmsnbc.com/id/25215605/\nEy doktor kardeşim, 3 senede ultrason zararlı diyen sen, şimdi çıkmışsın ve bu milletin gözünün içine baka baka ultrasonun hiç zararı yoktur diyorsun.\nBenim sana söyleyecek hiç sözüm yok.\nSeni yüce Rabbimle baş başa bırakıyorum. seni Allahımla baş başa bırakıyorum.","internal_url":"https://www.academia.edu/8203140/Bu_%C3%BClkede_b%C3%B6yle_doktorlar_var","translated_internal_url":"","created_at":"2014-09-04T18:26:40.598-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":820891,"coauthors_can_edit":true,"document_type":"other","co_author_tags":[],"downloadable_attachments":[],"slug":"Bu_ülkede_böyle_doktorlar_var","translated_slug":"","page_count":null,"language":"tr","content_type":"Work","owner":{"id":820891,"first_name":"Prof.Dr. İbrahim","middle_initials":"","last_name":"USLU","page_name":"ibrahimUSLU","domain_name":"gazi","created_at":"2011-10-07T03:26:52.651-07:00","display_name":"Prof.Dr. İbrahim USLU","url":"https://gazi.academia.edu/ibrahimUSLU"},"attachments":[],"research_interests":[],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="7718388"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/7718388/Sa%C3%A7_boyalar%C4%B1_kanser_yap%C4%B1yor_mu"><img alt="Research paper thumbnail of Saç boyaları kanser yapıyor mu?" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/7718388/Sa%C3%A7_boyalar%C4%B1_kanser_yap%C4%B1yor_mu">Saç boyaları kanser yapıyor mu?</a></div><div class="wp-workCard_item"><span>Hürriyet Gazetesi</span><span>, Jul 19, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrah...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, yapılan araştırmalarda, saç boyaları ile cilt, idrar kesesi, yumurtalık, lösemi, lenfoma, göğüs, beyin ve kan kanseri arasındaki ilişkilerin gözlendiğini söyledi. <br /> <br />Prof. Dr. İbrahim Uslu, Amerikan Kanser Cemiyeti&#39;ne göre saç boyalarında bulunan kimyasalların kanser oluşumunu tetikleyebildiğini söyledi. <br />Boyaların içerisinde bulunan, aromatik amin ve fenol adlı kimyasalların adeta bir sünger gibi olan saç derisinden geçerek deri içinde kanserojen etkiye sahip N-nitrozaminlere dönüştüğünü belirten Uslu, bu bileşiklerin kanser oluşumunu tetiklerken ilk olarak karaciğeri hedef aldığını vurguladı.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="7718388"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="7718388"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 7718388; 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Güçlü antioksidan etkisiyle kalp hastalıklarına karşı koruyucu etki gösterir. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="7127691"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/7127691/Maden_ocaklar%C4%B1ndaki_gizli_tehlike"><img alt="Research paper thumbnail of Maden ocaklarındaki gizli tehlike" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/7127691/Maden_ocaklar%C4%B1ndaki_gizli_tehlike">Maden ocaklarındaki gizli tehlike</a></div><div class="wp-workCard_item"><span>Sabah Gazetesi</span><span>, May 22, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Yeraltı maden ocaklarındaki en önemli radyasyon kaynağı olarak görülen &quot;radon gazı&quot;, renksiz, kok...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Yeraltı maden ocaklarındaki en önemli radyasyon kaynağı olarak görülen &quot;radon gazı&quot;, renksiz, kokusuz, tatsız ve radyoaktif bir gaz olduğundan, rezervlerde yeterli havalandırma yapılmadığında akciğer kanseri riskini artırıyor.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="7127691"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="7127691"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 7127691; 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Gazi Üniversitesi Gazi Eğitim Fakültesi Kimya Eğitimi Anabilim Dalı Öğretim Üyesi Prof. Dr. İbrahim Uslu, AA muhabirine yaptığı açıklamada, vücudun havadaki oksijen atomu ve onun benzeri serbest radikallerin her an saldırısına maruz kaldığını belirtti.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="6958810"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="6958810"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 6958810; 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