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js-work-card work_15135517 coauthored" data-work_id="15135517" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/15135517/Modelling_dynamic_behaviour_and_noise_generation_in_gear_pumps_Procedure_and_validation">Modelling dynamic behaviour and noise generation in gear pumps: Procedure and validation</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest">and sharing with colleagues.</div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/15135517" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" 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data-has-card-for-user="34173745" href="https://independent.academia.edu/EmilianoMucchi">Emiliano Mucchi</a><script data-card-contents-for-user="34173745" type="text/json">{"id":34173745,"first_name":"Emiliano","last_name":"Mucchi","domain_name":"independent","page_name":"EmilianoMucchi","display_name":"Emiliano Mucchi","profile_url":"https://independent.academia.edu/EmilianoMucchi?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-15135517">+1</span><div class="hidden js-additional-users-15135517"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://ferrara.academia.edu/GiorgioDalpiaz">Giorgio Dalpiaz</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-15135517'), placement: 'bottom', hide_delay: 200, html: true, 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class="u-positionAbsolute" data-has-card-for-ri-list="15135517"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a>, <script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1280929" rel="nofollow" href="https://www.academia.edu/Documents/in/Applied_Acoustics">Applied Acoustics</a><script data-card-contents-for-ri="1280929" type="text/json">{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=15135517]'), work: {"id":15135517,"title":"Modelling dynamic behaviour and noise generation in gear pumps: Procedure and validation","created_at":"2015-08-24T00:39:16.643-07:00","url":"https://www.academia.edu/15135517/Modelling_dynamic_behaviour_and_noise_generation_in_gear_pumps_Procedure_and_validation?f_ri=80799","dom_id":"work_15135517","summary":"and sharing with colleagues.","downloadable_attachments":[{"id":43547903,"asset_id":15135517,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":34173745,"first_name":"Emiliano","last_name":"Mucchi","domain_name":"independent","page_name":"EmilianoMucchi","display_name":"Emiliano Mucchi","profile_url":"https://independent.academia.edu/EmilianoMucchi?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":34177084,"first_name":"Giorgio","last_name":"Dalpiaz","domain_name":"ferrara","page_name":"GiorgioDalpiaz","display_name":"Giorgio Dalpiaz","profile_url":"https://ferrara.academia.edu/GiorgioDalpiaz?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_21214467 coauthored" data-work_id="21214467" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/21214467/Aircraft_noise_monitoring_according_to_ISO_20906_Evaluation_of_uncertainty_derived_from_the_human_factors_affecting_event_detection">Aircraft noise-monitoring according to ISO 20906: Evaluation of uncertainty derived from the human factors affecting event detection</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">One of the most important issues in aircraft noise monitoring systems is the correct detection and marking of aircraft sound events through their measurement profiles, as this influences the reported results. In the recent ISO 20906... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_21214467" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">One of the most important issues in aircraft noise monitoring systems is the correct detection and marking of aircraft sound events through their measurement profiles, as this influences the reported results. In the recent ISO 20906 (unattended monitoring of aircraft sound in the vicinity of airports) this marking task is split into: detection from the sound level time history, classification of probable aircraft sound events, and the concluding identification of aircraft sound events through non-acoustic features.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/21214467" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="e10ccca56b4d5f2e59b87e96fab8f101" rel="nofollow" data-download="{"attachment_id":41765820,"asset_id":21214467,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/41765820/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="6859851" href="https://upm-es.academia.edu/marianoruiz">mariano ruiz</a><script data-card-contents-for-user="6859851" type="text/json">{"id":6859851,"first_name":"mariano","last_name":"ruiz","domain_name":"upm-es","page_name":"marianoruiz","display_name":"mariano ruiz","profile_url":"https://upm-es.academia.edu/marianoruiz?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-21214467">+3</span><div class="hidden js-additional-users-21214467"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/JTrujillo2">J. Trujillo</a></span></div><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/RaulPagan">Raul Pagan</a></span></div><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://upm-es.academia.edu/C%C3%A9sarAsensio">César Asensio</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-21214467'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-21214467').html(); } } new HoverPopover(popoverSettings); })();</script></li><li class="js-paper-rank-work_21214467 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="21214467"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 21214467, container: ".js-paper-rank-work_21214467", }); });</script></li><li class="js-percentile-work_21214467 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 21214467; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_21214467"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_21214467 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="21214467"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 21214467; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=21214467]").text(description); $(".js-view-count-work_21214467").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_21214467").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="21214467"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a>, <script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1280929" rel="nofollow" href="https://www.academia.edu/Documents/in/Applied_Acoustics">Applied Acoustics</a><script data-card-contents-for-ri="1280929" type="text/json">{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=21214467]'), work: {"id":21214467,"title":"Aircraft noise-monitoring according to ISO 20906: Evaluation of uncertainty derived from the human factors affecting event detection","created_at":"2016-01-30T01:16:01.866-08:00","url":"https://www.academia.edu/21214467/Aircraft_noise_monitoring_according_to_ISO_20906_Evaluation_of_uncertainty_derived_from_the_human_factors_affecting_event_detection?f_ri=80799","dom_id":"work_21214467","summary":"One of the most important issues in aircraft noise monitoring systems is the correct detection and marking of aircraft sound events through their measurement profiles, as this influences the reported results. In the recent ISO 20906 (unattended monitoring of aircraft sound in the vicinity of airports) this marking task is split into: detection from the sound level time history, classification of probable aircraft sound events, and the concluding identification of aircraft sound events through non-acoustic features.","downloadable_attachments":[{"id":41765820,"asset_id":21214467,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":6859851,"first_name":"mariano","last_name":"ruiz","domain_name":"upm-es","page_name":"marianoruiz","display_name":"mariano ruiz","profile_url":"https://upm-es.academia.edu/marianoruiz?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":42580738,"first_name":"J.","last_name":"Trujillo","domain_name":"independent","page_name":"JTrujillo2","display_name":"J. Trujillo","profile_url":"https://independent.academia.edu/JTrujillo2?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":42454209,"first_name":"Raul","last_name":"Pagan","domain_name":"independent","page_name":"RaulPagan","display_name":"Raul Pagan","profile_url":"https://independent.academia.edu/RaulPagan?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":6657358,"first_name":"César","last_name":"Asensio","domain_name":"upm-es","page_name":"CésarAsensio","display_name":"César Asensio","profile_url":"https://upm-es.academia.edu/C%C3%A9sarAsensio?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_25673005" data-work_id="25673005" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/25673005/Vapour_liquid_equilibrium_compositional_data_for_a_model_fluid_at_elevated_temperatures_and_pressures">Vapour–liquid equilibrium compositional data for a model fluid at elevated temperatures and pressures</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Direct composition measurements are made on equilibrium vapour and liquid phases of a five-component model gas condensate sample. The compositions of equilibrium phases are measured at two temperatures (303.15 and 353.15 K) and pressures... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_25673005" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Direct composition measurements are made on equilibrium vapour and liquid phases of a five-component model gas condensate sample. The compositions of equilibrium phases are measured at two temperatures (303.15 and 353.15 K) and pressures of 30.44-19.41 MPa. Component balance calculations and evaluation of the internal consistency of the measured equilibrium ratios of components demonstrate the reliability of measurements.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/25673005" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="94d195178e495699452c67d2b8779381" rel="nofollow" data-download="{"attachment_id":46013062,"asset_id":25673005,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/46013062/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="49306155" href="https://independent.academia.edu/BahmanTohidi">Bahman Tohidi</a><script data-card-contents-for-user="49306155" type="text/json">{"id":49306155,"first_name":"Bahman","last_name":"Tohidi","domain_name":"independent","page_name":"BahmanTohidi","display_name":"Bahman Tohidi","profile_url":"https://independent.academia.edu/BahmanTohidi?f_ri=80799","photo":"https://0.academia-photos.com/49306155/12978887/14339331/s65_bahman.tohidi.png"}</script></span></span></li><li class="js-paper-rank-work_25673005 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="25673005"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 25673005, container: ".js-paper-rank-work_25673005", }); });</script></li><li class="js-percentile-work_25673005 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 25673005; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_25673005"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_25673005 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="25673005"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 25673005; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=25673005]").text(description); $(".js-view-count-work_25673005").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_25673005").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="25673005"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">6</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="629119" rel="nofollow" href="https://www.academia.edu/Documents/in/Fluid_phase_equilibria">Fluid phase equilibria</a>, <script data-card-contents-for-ri="629119" type="text/json">{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="965508" rel="nofollow" href="https://www.academia.edu/Documents/in/Compositional_Data">Compositional Data</a><script data-card-contents-for-ri="965508" type="text/json">{"id":965508,"name":"Compositional Data","url":"https://www.academia.edu/Documents/in/Compositional_Data?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=25673005]'), work: {"id":25673005,"title":"Vapour–liquid equilibrium compositional data for a model fluid at elevated temperatures and pressures","created_at":"2016-05-28T01:55:03.226-07:00","url":"https://www.academia.edu/25673005/Vapour_liquid_equilibrium_compositional_data_for_a_model_fluid_at_elevated_temperatures_and_pressures?f_ri=80799","dom_id":"work_25673005","summary":"Direct composition measurements are made on equilibrium vapour and liquid phases of a five-component model gas condensate sample. The compositions of equilibrium phases are measured at two temperatures (303.15 and 353.15 K) and pressures of 30.44-19.41 MPa. Component balance calculations and evaluation of the internal consistency of the measured equilibrium ratios of components demonstrate the reliability of measurements.","downloadable_attachments":[{"id":46013062,"asset_id":25673005,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":49306155,"first_name":"Bahman","last_name":"Tohidi","domain_name":"independent","page_name":"BahmanTohidi","display_name":"Bahman Tohidi","profile_url":"https://independent.academia.edu/BahmanTohidi?f_ri=80799","photo":"https://0.academia-photos.com/49306155/12978887/14339331/s65_bahman.tohidi.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true},{"id":965508,"name":"Compositional Data","url":"https://www.academia.edu/Documents/in/Compositional_Data?f_ri=80799","nofollow":true},{"id":1068737,"name":"Elevated Temperature","url":"https://www.academia.edu/Documents/in/Elevated_Temperature?f_ri=80799"},{"id":2007534,"name":"Component Model","url":"https://www.academia.edu/Documents/in/Component_Model?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_81344820" data-work_id="81344820" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/81344820/Investigation_of_Perceptual_Interaural_Time_Difference_Evaluation_Protocols_in_a_Binaural_Context">Investigation of Perceptual Interaural Time Difference Evaluation Protocols in a Binaural Context</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">We report the advantages and drawbacks of three protocols (adjustment, AFC-yes/no, and AFC-left/right discrimination protocols)e valuating the estimation of the interaural time differences (ITDs)f or correct lateralization perception. The... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_81344820" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">We report the advantages and drawbacks of three protocols (adjustment, AFC-yes/no, and AFC-left/right discrimination protocols)e valuating the estimation of the interaural time differences (ITDs)f or correct lateralization perception. The protocols were compared with respect to reliability of the perceivedITD and just noticeable difference (JND)e stimations, robustness to participants' errors, effect of the number of tested blocks of trials, and test duration. Binaural stimuli were employed, including all spatial cues for sound sources placed at horizontal positions of 30 • and 90 • .All three protocols yielded comparable perceivedITD butdifferent JNDs at 30 •. At 90 • ,b oth the AFC-left/right and the adjustment protocols were more problematic than the yes/no protocol. Overall, only the yes/no protocol fulfilled the requirements of this study,i.e. aquick protocol that can be used for all angles.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/81344820" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="1a9f9d6e0b96998f9d1723b8dc40cbf8" rel="nofollow" data-download="{"attachment_id":87420394,"asset_id":81344820,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/87420394/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39373832" href="https://sorbonne-fr.academia.edu/BrianKatz">Brian F G Katz</a><script data-card-contents-for-user="39373832" type="text/json">{"id":39373832,"first_name":"Brian","last_name":"Katz","domain_name":"sorbonne-fr","page_name":"BrianKatz","display_name":"Brian F G Katz","profile_url":"https://sorbonne-fr.academia.edu/BrianKatz?f_ri=80799","photo":"https://0.academia-photos.com/39373832/12066143/37315216/s65_brian.katz.jpg"}</script></span></span></li><li class="js-paper-rank-work_81344820 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="81344820"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 81344820, container: ".js-paper-rank-work_81344820", }); 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$(".js-view-count[data-work-id=81344820]").text(description); $(".js-view-count-work_81344820").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_81344820").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="81344820"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="300" rel="nofollow" href="https://www.academia.edu/Documents/in/Mathematics">Mathematics</a>, <script data-card-contents-for-ri="300" type="text/json">{"id":300,"name":"Mathematics","url":"https://www.academia.edu/Documents/in/Mathematics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="867" rel="nofollow" href="https://www.academia.edu/Documents/in/Perception">Perception</a>, <script data-card-contents-for-ri="867" type="text/json">{"id":867,"name":"Perception","url":"https://www.academia.edu/Documents/in/Perception?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=81344820]'), work: {"id":81344820,"title":"Investigation of Perceptual Interaural Time Difference Evaluation Protocols in a Binaural Context","created_at":"2022-06-12T21:59:04.536-07:00","url":"https://www.academia.edu/81344820/Investigation_of_Perceptual_Interaural_Time_Difference_Evaluation_Protocols_in_a_Binaural_Context?f_ri=80799","dom_id":"work_81344820","summary":"We report the advantages and drawbacks of three protocols (adjustment, AFC-yes/no, and AFC-left/right discrimination protocols)e valuating the estimation of the interaural time differences (ITDs)f or correct lateralization perception. The protocols were compared with respect to reliability of the perceivedITD and just noticeable difference (JND)e stimations, robustness to participants' errors, effect of the number of tested blocks of trials, and test duration. Binaural stimuli were employed, including all spatial cues for sound sources placed at horizontal positions of 30 • and 90 • .All three protocols yielded comparable perceivedITD butdifferent JNDs at 30 •. At 90 • ,b oth the AFC-left/right and the adjustment protocols were more problematic than the yes/no protocol. Overall, only the yes/no protocol fulfilled the requirements of this study,i.e. aquick protocol that can be used for all angles.","downloadable_attachments":[{"id":87420394,"asset_id":81344820,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39373832,"first_name":"Brian","last_name":"Katz","domain_name":"sorbonne-fr","page_name":"BrianKatz","display_name":"Brian F G Katz","profile_url":"https://sorbonne-fr.academia.edu/BrianKatz?f_ri=80799","photo":"https://0.academia-photos.com/39373832/12066143/37315216/s65_brian.katz.jpg"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":300,"name":"Mathematics","url":"https://www.academia.edu/Documents/in/Mathematics?f_ri=80799","nofollow":true},{"id":867,"name":"Perception","url":"https://www.academia.edu/Documents/in/Perception?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":294592,"name":"Binaural Recording","url":"https://www.academia.edu/Documents/in/Binaural_Recording?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_71790004" data-work_id="71790004" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" rel="nofollow" href="https://www.academia.edu/71790004/Study_of_the_effectiveness_of_electric_vehicle_warning_sounds_depending_on_the_urban_environment">Study of the effectiveness of electric vehicle warning sounds depending on the urban environment</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Abstract Electric and Hybrid Electric vehicles (EV and HEV) seem to be the future of transport in smart cities and the key for the total reduction of noise disturbance and pollution in urban areas. However, several problems have to be... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_71790004" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Abstract Electric and Hybrid Electric vehicles (EV and HEV) seem to be the future of transport in smart cities and the key for the total reduction of noise disturbance and pollution in urban areas. However, several problems have to be solved to guarantee the safety of these types of vehicle. Up to now, the use of HEV has shown the dangers of a “quiet” transport system in urban environments; in fact, it has been estimated that an HEV is twice as likely to be involved in a pedestrian crash as would be an internal combustion engine (ICE) vehicle in the same situation. With the aim of improving their safety, different kinds of warning sounds are being designed to increase the detectability of EV and HEV without themselves becoming new annoying sound sources. The sound directivity, frequency of emission and intensity of warning sound systems will guarantee their efficiency and limited noise impact. Several research works bring to the fore a significant variation of the pedestrian response time to different acoustic stimuli. However, it is necessary to examine the suitability of these warning sounds according to the urban environments in which they are going to be emitted. Distinct areas inside the city have different soundscapes whose spectral content can vary significantly, masking some of the sounds suggested as an alert. This paper analyses in detail the main characteristics of several warning sounds proposed by the industry, conducting a comparative study of the different design trends. A total of 131 sighted listeners were exposed to a virtual road-crossing test. The behaviour and appropriateness of warning sounds are analysed depending on the urban environment. For this purpose, three clearly different soundscapes have been selected: stopped vehicles at a traffic light, a pedestrian shopping area and the vicinity of a playground. The results highlight the wide variability in pedestrian reaction time for the different warning sounds used. Some signals considerably improve the detectability of the vehicle, providing results even above the ICE vehicle ones. However, other warning sounds do not decrease the reaction time with respect to the EV. In addition, a clear dependence is observed between the detectability and the soundscape involved, changing the results for the same warning sound depending on the acoustic environment.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/71790004" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="120579090" href="https://independent.academia.edu/MLLORETCLIMENT">MIGUEL LLORET CLIMENT</a><script data-card-contents-for-user="120579090" type="text/json">{"id":120579090,"first_name":"MIGUEL","last_name":"LLORET CLIMENT","domain_name":"independent","page_name":"MLLORETCLIMENT","display_name":"MIGUEL LLORET CLIMENT","profile_url":"https://independent.academia.edu/MLLORETCLIMENT?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_71790004 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="71790004"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 71790004, container: ".js-paper-rank-work_71790004", }); 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$(".js-view-count[data-work-id=71790004]").text(description); $(".js-view-count-work_71790004").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_71790004").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="71790004"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="48" rel="nofollow" href="https://www.academia.edu/Documents/in/Engineering">Engineering</a>, <script data-card-contents-for-ri="48" type="text/json">{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a>, <script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=71790004]'), work: {"id":71790004,"title":"Study of the effectiveness of electric vehicle warning sounds depending on the urban environment","created_at":"2022-02-18T00:05:31.412-08:00","url":"https://www.academia.edu/71790004/Study_of_the_effectiveness_of_electric_vehicle_warning_sounds_depending_on_the_urban_environment?f_ri=80799","dom_id":"work_71790004","summary":"Abstract Electric and Hybrid Electric vehicles (EV and HEV) seem to be the future of transport in smart cities and the key for the total reduction of noise disturbance and pollution in urban areas. However, several problems have to be solved to guarantee the safety of these types of vehicle. Up to now, the use of HEV has shown the dangers of a “quiet” transport system in urban environments; in fact, it has been estimated that an HEV is twice as likely to be involved in a pedestrian crash as would be an internal combustion engine (ICE) vehicle in the same situation. With the aim of improving their safety, different kinds of warning sounds are being designed to increase the detectability of EV and HEV without themselves becoming new annoying sound sources. The sound directivity, frequency of emission and intensity of warning sound systems will guarantee their efficiency and limited noise impact. Several research works bring to the fore a significant variation of the pedestrian response time to different acoustic stimuli. However, it is necessary to examine the suitability of these warning sounds according to the urban environments in which they are going to be emitted. Distinct areas inside the city have different soundscapes whose spectral content can vary significantly, masking some of the sounds suggested as an alert. This paper analyses in detail the main characteristics of several warning sounds proposed by the industry, conducting a comparative study of the different design trends. A total of 131 sighted listeners were exposed to a virtual road-crossing test. The behaviour and appropriateness of warning sounds are analysed depending on the urban environment. For this purpose, three clearly different soundscapes have been selected: stopped vehicles at a traffic light, a pedestrian shopping area and the vicinity of a playground. The results highlight the wide variability in pedestrian reaction time for the different warning sounds used. Some signals considerably improve the detectability of the vehicle, providing results even above the ICE vehicle ones. However, other warning sounds do not decrease the reaction time with respect to the EV. In addition, a clear dependence is observed between the detectability and the soundscape involved, changing the results for the same warning sound depending on the acoustic environment.","downloadable_attachments":[],"ordered_authors":[{"id":120579090,"first_name":"MIGUEL","last_name":"LLORET CLIMENT","domain_name":"independent","page_name":"MLLORETCLIMENT","display_name":"MIGUEL LLORET CLIMENT","profile_url":"https://independent.academia.edu/MLLORETCLIMENT?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=80799","nofollow":true},{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_62942006" data-work_id="62942006" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/62942006/High_density_high_performance_high_confinement_mode_plasmas_in_the_Joint_European_Torus_JET_">High density, high performance high-confinement-mode plasmas in the Joint European Torus (JET)</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/62942006" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="11237703523c22efc91cc4e56b6069e0" rel="nofollow" data-download="{"attachment_id":75541963,"asset_id":62942006,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/75541963/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="44142776" href="https://independent.academia.edu/FSartori2">F. 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The performance of the algorithm was tested both by... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47441664" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The paper presents the results of applying nonlocal means (NLMs) approach in the problem of separating respiration and cardiac sounds in a signal recorded on a human chest wall. The performance of the algorithm was tested both by simulated and real signals. As a quantitative efficiency measure of NLM filtra tion, the angle of divergence between isolated and reference signal was used. It is shown that for a wide range of signal to noise ratios, the algorithm makes it possible to efficiently solve this problem of separating cardiac and respiration sounds in the sum signal recorded on a human chest wall.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/47441664" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="53bf99ece56600fc783e04a5fd5754c4" rel="nofollow" data-download="{"attachment_id":66532814,"asset_id":47441664,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/66532814/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="42148496" href="https://independent.academia.edu/RuAlex">Alex Ru</a><script data-card-contents-for-user="42148496" type="text/json">{"id":42148496,"first_name":"Alex","last_name":"Ru","domain_name":"independent","page_name":"RuAlex","display_name":"Alex Ru","profile_url":"https://independent.academia.edu/RuAlex?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_47441664 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="47441664"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 47441664, container: ".js-paper-rank-work_47441664", }); });</script></li><li class="js-percentile-work_47441664 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 47441664; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_47441664"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_47441664 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="47441664"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 47441664; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=47441664]").text(description); $(".js-view-count-work_47441664").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_47441664").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="47441664"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=47441664]'), work: {"id":47441664,"title":"Using nonlocal means to separate cardiac and respiration sounds","created_at":"2021-04-22T06:40:50.202-07:00","url":"https://www.academia.edu/47441664/Using_nonlocal_means_to_separate_cardiac_and_respiration_sounds?f_ri=80799","dom_id":"work_47441664","summary":"The paper presents the results of applying nonlocal means (NLMs) approach in the problem of separating respiration and cardiac sounds in a signal recorded on a human chest wall. The performance of the algorithm was tested both by simulated and real signals. As a quantitative efficiency measure of NLM filtra tion, the angle of divergence between isolated and reference signal was used. It is shown that for a wide range of signal to noise ratios, the algorithm makes it possible to efficiently solve this problem of separating cardiac and respiration sounds in the sum signal recorded on a human chest wall.","downloadable_attachments":[{"id":66532814,"asset_id":47441664,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":42148496,"first_name":"Alex","last_name":"Ru","domain_name":"independent","page_name":"RuAlex","display_name":"Alex Ru","profile_url":"https://independent.academia.edu/RuAlex?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_3559363" data-work_id="3559363" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/3559363/Application_of_Artificial_Neural_Networks_for_Childhood_Obesity_Predicition">Application of Artificial Neural Networks for Childhood Obesity Predicition</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In this study, artificial neural networks (ANNs) were applied to predict the mean monthly wind speed of any target station using the mean monthly wind speeds of neighboring stations which are indicated as reference stations. Hourly wind... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_3559363" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In this study, artificial neural networks (ANNs) were applied to predict the mean monthly wind speed of any target station using the mean monthly wind speeds of neighboring stations which are indicated as reference stations. Hourly wind speed data, collected by the Turkish State Meteorological Service (TSMS) at 8 measuring stations located in the eastern Mediterranean region of Turkey were used. The long-term wind data, containing hourly wind speeds, directions and related information, cover the period between 1992 and 2001. These data were divided into two sections. According to the correlation coefficients, reference and target stations were defined. The mean monthly wind speeds of reference stations were used and also corresponding months were specified in the input layer of the network. On the other hand, the mean monthly wind speed of the target station was utilized in the output layer of the network. Resilient propagation (RP) learning algorithm was applied in the present simulation. The hidden layers and output layer of the network consist of logistic sigmoid transfer function (logsig) and linear transfer function (purelin) as an activation function. Finally, the values determined by ANN model were compared with the actual data. The maximum mean absolute percentage error was found to be 14.13% for Antakya meteorological station and the best result was found to be 4.49% for Mersin meteorological station. r</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/3559363" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="3ffbeb30e0c79900cb14f40b4f957723" rel="nofollow" data-download="{"attachment_id":50230956,"asset_id":3559363,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/50230956/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="4229567" href="https://uni-mb.academia.edu/MartinBigec">Martin Bigec</a><script data-card-contents-for-user="4229567" type="text/json">{"id":4229567,"first_name":"Martin","last_name":"Bigec","domain_name":"uni-mb","page_name":"MartinBigec","display_name":"Martin Bigec","profile_url":"https://uni-mb.academia.edu/MartinBigec?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_3559363 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="3559363"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 3559363, container: ".js-paper-rank-work_3559363", }); 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Hourly wind speed data, collected by the Turkish State Meteorological Service (TSMS) at 8 measuring stations located in the eastern Mediterranean region of Turkey were used. The long-term wind data, containing hourly wind speeds, directions and related information, cover the period between 1992 and 2001. These data were divided into two sections. According to the correlation coefficients, reference and target stations were defined. The mean monthly wind speeds of reference stations were used and also corresponding months were specified in the input layer of the network. On the other hand, the mean monthly wind speed of the target station was utilized in the output layer of the network. Resilient propagation (RP) learning algorithm was applied in the present simulation. The hidden layers and output layer of the network consist of logistic sigmoid transfer function (logsig) and linear transfer function (purelin) as an activation function. Finally, the values determined by ANN model were compared with the actual data. The maximum mean absolute percentage error was found to be 14.13% for Antakya meteorological station and the best result was found to be 4.49% for Mersin meteorological station. r","downloadable_attachments":[{"id":50230956,"asset_id":3559363,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":4229567,"first_name":"Martin","last_name":"Bigec","domain_name":"uni-mb","page_name":"MartinBigec","display_name":"Martin Bigec","profile_url":"https://uni-mb.academia.edu/MartinBigec?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":73,"name":"Civil Engineering","url":"https://www.academia.edu/Documents/in/Civil_Engineering?f_ri=80799","nofollow":true},{"id":237,"name":"Cognitive 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u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_5423524" data-work_id="5423524" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/5423524/Scaling_laws_of_resistive_magnetohydrodynamic_reconnection_in_the_high_Lundquist_number_plasmoid_unstable_regime">Scaling laws of resistive magnetohydrodynamic reconnection in the high-Lundquist-number, plasmoid-unstable regime</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The Sweet-Parker layer in a system that exceeds a critical value of the Lundquist number ͑S͒ is unstable to the plasmoid instability. In this paper, a numerical scaling study has been done with an island coalescing system driven by a low... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_5423524" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The Sweet-Parker layer in a system that exceeds a critical value of the Lundquist number ͑S͒ is unstable to the plasmoid instability. In this paper, a numerical scaling study has been done with an island coalescing system driven by a low level of random noise. In the early stage, a primary Sweet-Parker layer forms between the two coalescing islands. The primary Sweet-Parker layer breaks into multiple plasmoids and even thinner current sheets through multiple levels of cascading if the Lundquist number is greater than a critical value S c Ӎ 4 ϫ 10 4 . As a result of the plasmoid instability, the system realizes a fast nonlinear reconnection rate that is nearly independent of S, and is only weakly dependent on the level of noise. The number of plasmoids in the linear regime is found to scales as S 3/8 , as predicted by an earlier asymptotic analysis ͓N. F. Loureiro et al., Phys. Plasmas 14, 100703 ͑2007͔͒. In the nonlinear regime, the number of plasmoids follows a steeper scaling, and is proportional to S. The thickness and length of current sheets are found to scale as S −1 , and the local current densities of current sheets scale as S −1 . Heuristic arguments are given in support of theses scaling relations.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/5423524" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="14ea2b9e2e8235deb131f8136b3babb8" rel="nofollow" data-download="{"attachment_id":49298553,"asset_id":5423524,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/49298553/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="7581378" href="https://princeton.academia.edu/YiMinHuang">Yi-Min Huang</a><script data-card-contents-for-user="7581378" type="text/json">{"id":7581378,"first_name":"Yi-Min","last_name":"Huang","domain_name":"princeton","page_name":"YiMinHuang","display_name":"Yi-Min Huang","profile_url":"https://princeton.academia.edu/YiMinHuang?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_5423524 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="5423524"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 5423524, container: ".js-paper-rank-work_5423524", }); 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In this paper, a numerical scaling study has been done with an island coalescing system driven by a low level of random noise. In the early stage, a primary Sweet-Parker layer forms between the two coalescing islands. The primary Sweet-Parker layer breaks into multiple plasmoids and even thinner current sheets through multiple levels of cascading if the Lundquist number is greater than a critical value S c Ӎ 4 ϫ 10 4 . As a result of the plasmoid instability, the system realizes a fast nonlinear reconnection rate that is nearly independent of S, and is only weakly dependent on the level of noise. The number of plasmoids in the linear regime is found to scales as S 3/8 , as predicted by an earlier asymptotic analysis ͓N. F. Loureiro et al., Phys. Plasmas 14, 100703 ͑2007͔͒. In the nonlinear regime, the number of plasmoids follows a steeper scaling, and is proportional to S. The thickness and length of current sheets are found to scale as S −1 , and the local current densities of current sheets scale as S −1 . Heuristic arguments are given in support of theses scaling relations.","downloadable_attachments":[{"id":49298553,"asset_id":5423524,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":7581378,"first_name":"Yi-Min","last_name":"Huang","domain_name":"princeton","page_name":"YiMinHuang","display_name":"Yi-Min Huang","profile_url":"https://princeton.academia.edu/YiMinHuang?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":721,"name":"Magnetohydrodynamics","url":"https://www.academia.edu/Documents/in/Magnetohydrodynamics?f_ri=80799","nofollow":true},{"id":60653,"name":"Transport Properties","url":"https://www.academia.edu/Documents/in/Transport_Properties?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":121397,"name":"Magnetic Reconnection","url":"https://www.academia.edu/Documents/in/Magnetic_Reconnection?f_ri=80799","nofollow":true},{"id":173959,"name":"Current Density","url":"https://www.academia.edu/Documents/in/Current_Density?f_ri=80799"},{"id":250422,"name":"Random Noise","url":"https://www.academia.edu/Documents/in/Random_Noise?f_ri=80799"},{"id":277944,"name":"asymptotic Analysis","url":"https://www.academia.edu/Documents/in/asymptotic_Analysis?f_ri=80799"},{"id":778976,"name":"Scaling Law","url":"https://www.academia.edu/Documents/in/Scaling_Law?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_27218795" data-work_id="27218795" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/27218795/On_volume_translations_in_equations_of_state">On volume translations in equations of state</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Translations are often applied on equations of state with the aim of improving the description of molar volumes. In the present note an alternative presentation of the ideas developed in the pioneering work of Ptneloux and Rauzy... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_27218795" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Translations are often applied on equations of state with the aim of improving the description of molar volumes. In the present note an alternative presentation of the ideas developed in the pioneering work of Ptneloux and Rauzy [PCneloux, A., E. Rauzy, A consistent correction for Redlich-Kwong-Soave volumes. Fluid Phase Equilib., 8 (1982) 7-23.1 is provided and some issues are discussed in a deeper level of detail. 0 1997 Elsevier Science B.V. Key~~wds: Model; Equation of state; Volume; Vapor pressure; Mixture: Translations * Corresponding author 0378.3812/97/$17.00 0 1997 Elsevier Science B.V. All rights reserved. /'II s037x-~x12(97)00185-4</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/27218795" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="c82f06c23f4df4c2434ebc188605db68" rel="nofollow" data-download="{"attachment_id":47475847,"asset_id":27218795,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/47475847/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="51302004" href="https://independent.academia.edu/EstebanBrignole">Esteban Brignole</a><script data-card-contents-for-user="51302004" type="text/json">{"id":51302004,"first_name":"Esteban","last_name":"Brignole","domain_name":"independent","page_name":"EstebanBrignole","display_name":"Esteban Brignole","profile_url":"https://independent.academia.edu/EstebanBrignole?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_27218795 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="27218795"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 27218795, container: ".js-paper-rank-work_27218795", }); 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In the present note an alternative presentation of the ideas developed in the pioneering work of Ptneloux and Rauzy [PCneloux, A., E. Rauzy, A consistent correction for Redlich-Kwong-Soave volumes. Fluid Phase Equilib., 8 (1982) 7-23.1 is provided and some issues are discussed in a deeper level of detail. 0 1997 Elsevier Science B.V. Key~~wds: Model; Equation of state; Volume; Vapor pressure; Mixture: Translations * Corresponding author 0378.3812/97/$17.00 0 1997 Elsevier Science B.V. All rights reserved. /'II s037x-~x12(97)00185-4","downloadable_attachments":[{"id":47475847,"asset_id":27218795,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":51302004,"first_name":"Esteban","last_name":"Brignole","domain_name":"independent","page_name":"EstebanBrignole","display_name":"Esteban Brignole","profile_url":"https://independent.academia.edu/EstebanBrignole?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":30718,"name":"Level Of Detail (LOD)","url":"https://www.academia.edu/Documents/in/Level_Of_Detail_LOD_?f_ri=80799","nofollow":true},{"id":61684,"name":"Model","url":"https://www.academia.edu/Documents/in/Model?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":114713,"name":"Vapor Pressure","url":"https://www.academia.edu/Documents/in/Vapor_Pressure?f_ri=80799"},{"id":143335,"name":"Volume","url":"https://www.academia.edu/Documents/in/Volume?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"},{"id":1014403,"name":"Mixture","url":"https://www.academia.edu/Documents/in/Mixture?f_ri=80799"},{"id":1320599,"name":"Equation of State","url":"https://www.academia.edu/Documents/in/Equation_of_State?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_27118340" data-work_id="27118340" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/27118340/Drift_wave_test_particle_transport_in_reversed_shear_profile">Drift wave test particle transport in reversed shear profile</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Drift wave maps, area preserving maps that describe the motion of charged particles in drift waves, are derived. The maps allow the integration of particle orbits on the long time scale needed to describe transport. Calculations using the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_27118340" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Drift wave maps, area preserving maps that describe the motion of charged particles in drift waves, are derived. The maps allow the integration of particle orbits on the long time scale needed to describe transport. Calculations using the drift wave maps show that dramatic improvement in the particle confinement, in the presence of a given level and spectrum of EϫB turbulence, can occur for q(r) profiles with reversed shear. A similar reduction in the transport, i.e., one that is independent of the turbulence, is observed in the presence of an equilibrium radial electric field with shear. The transport reduction, caused by the combined effects of radial electric field shear and both monotonic and reversed shear magnetic q profiles, is also investigated.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/27118340" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="979cc3b03802f6f195c0dd047883698e" rel="nofollow" data-download="{"attachment_id":47369235,"asset_id":27118340,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/47369235/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="48029487" href="https://victoria.academia.edu/PhilipMorrison">Philip S Morrison</a><script data-card-contents-for-user="48029487" type="text/json">{"id":48029487,"first_name":"Philip","last_name":"Morrison","domain_name":"victoria","page_name":"PhilipMorrison","display_name":"Philip S Morrison","profile_url":"https://victoria.academia.edu/PhilipMorrison?f_ri=80799","photo":"https://0.academia-photos.com/48029487/12651420/14073509/s65_philip.morrison.jpg"}</script></span></span></li><li class="js-paper-rank-work_27118340 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="27118340"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 27118340, container: ".js-paper-rank-work_27118340", }); 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The maps allow the integration of particle orbits on the long time scale needed to describe transport. Calculations using the drift wave maps show that dramatic improvement in the particle confinement, in the presence of a given level and spectrum of EϫB turbulence, can occur for q(r) profiles with reversed shear. A similar reduction in the transport, i.e., one that is independent of the turbulence, is observed in the presence of an equilibrium radial electric field with shear. The transport reduction, caused by the combined effects of radial electric field shear and both monotonic and reversed shear magnetic q profiles, is also investigated.","downloadable_attachments":[{"id":47369235,"asset_id":27118340,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":48029487,"first_name":"Philip","last_name":"Morrison","domain_name":"victoria","page_name":"PhilipMorrison","display_name":"Philip S Morrison","profile_url":"https://victoria.academia.edu/PhilipMorrison?f_ri=80799","photo":"https://0.academia-photos.com/48029487/12651420/14073509/s65_philip.morrison.jpg"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=80799","nofollow":true},{"id":517,"name":"Plasma Physics","url":"https://www.academia.edu/Documents/in/Plasma_Physics?f_ri=80799","nofollow":true},{"id":2024,"name":"Mass Transfer","url":"https://www.academia.edu/Documents/in/Mass_Transfer?f_ri=80799","nofollow":true},{"id":2802,"name":"Turbulence","url":"https://www.academia.edu/Documents/in/Turbulence?f_ri=80799","nofollow":true},{"id":5495,"name":"Wave turbulence","url":"https://www.academia.edu/Documents/in/Wave_turbulence?f_ri=80799"},{"id":34754,"name":"Magnetic field","url":"https://www.academia.edu/Documents/in/Magnetic_field?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":321836,"name":"Spectrum","url":"https://www.academia.edu/Documents/in/Spectrum?f_ri=80799"},{"id":775583,"name":"Shear","url":"https://www.academia.edu/Documents/in/Shear?f_ri=80799"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field?f_ri=80799"},{"id":1760204,"name":"Elementary Particles","url":"https://www.academia.edu/Documents/in/Elementary_Particles?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_25456048" data-work_id="25456048" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/25456048/The_problem_of_analytical_calculation_of_barrier_crossing_characteristics_for_L%C3%A9vy_flights">The problem of analytical calculation of barrier crossing characteristics for Lévy flights</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">By using the backward fractional Fokker-Planck equation we investigate the barrier crossing event in the presence of Lévy noise. After shortly review recent results obtained with different approaches on the time characteristics of the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_25456048" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">By using the backward fractional Fokker-Planck equation we investigate the barrier crossing event in the presence of Lévy noise. After shortly review recent results obtained with different approaches on the time characteristics of the barrier crossing, we derive a general differential equation useful to calculate the nonlinear relaxation time. We obtain analytically the nonlinear relaxation time for free Lévy flights and a closed expression in quadrature of the same characteristics for cubic potential.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/25456048" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5f387a178e6b516de9649dda3476a8b5" rel="nofollow" data-download="{"attachment_id":45773817,"asset_id":25456048,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/45773817/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="48958377" href="https://independent.academia.edu/AlexanderDubkov">Alexander Dubkov</a><script data-card-contents-for-user="48958377" type="text/json">{"id":48958377,"first_name":"Alexander","last_name":"Dubkov","domain_name":"independent","page_name":"AlexanderDubkov","display_name":"Alexander Dubkov","profile_url":"https://independent.academia.edu/AlexanderDubkov?f_ri=80799","photo":"https://0.academia-photos.com/48958377/12881815/14273797/s65_alexander.dubkov.jpg"}</script></span></span></li><li class="js-paper-rank-work_25456048 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="25456048"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 25456048, container: ".js-paper-rank-work_25456048", }); 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After shortly review recent results obtained with different approaches on the time characteristics of the barrier crossing, we derive a general differential equation useful to calculate the nonlinear relaxation time. We obtain analytically the nonlinear relaxation time for free Lévy flights and a closed expression in quadrature of the same characteristics for cubic potential.","downloadable_attachments":[{"id":45773817,"asset_id":25456048,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":48958377,"first_name":"Alexander","last_name":"Dubkov","domain_name":"independent","page_name":"AlexanderDubkov","display_name":"Alexander Dubkov","profile_url":"https://independent.academia.edu/AlexanderDubkov?f_ri=80799","photo":"https://0.academia-photos.com/48958377/12881815/14273797/s65_alexander.dubkov.jpg"}],"research_interests":[{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_22205436" data-work_id="22205436" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/22205436/An_extended_saturated_liquid_density_equation">An extended saturated liquid density equation</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/22205436" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="1f8e1afe1e150da230ba5c840a1e4a32" rel="nofollow" data-download="{"attachment_id":42859686,"asset_id":22205436,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/42859686/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="35867874" href="https://sharif.academia.edu/ShahabAyatollahi">Shahab Ayatollahi</a><script data-card-contents-for-user="35867874" type="text/json">{"id":35867874,"first_name":"Shahab","last_name":"Ayatollahi","domain_name":"sharif","page_name":"ShahabAyatollahi","display_name":"Shahab Ayatollahi","profile_url":"https://sharif.academia.edu/ShahabAyatollahi?f_ri=80799","photo":"https://0.academia-photos.com/35867874/11615910/12953230/s65_shahab.ayatollahi.jpg"}</script></span></span></li><li class="js-paper-rank-work_22205436 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="22205436"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 22205436, container: ".js-paper-rank-work_22205436", }); 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$(".js-view-count[data-work-id=22205436]").text(description); $(".js-view-count-work_22205436").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_22205436").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="22205436"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="629119" rel="nofollow" href="https://www.academia.edu/Documents/in/Fluid_phase_equilibria">Fluid phase equilibria</a>, <script data-card-contents-for-ri="629119" type="text/json">{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1120502" rel="nofollow" href="https://www.academia.edu/Documents/in/Experimental_Data">Experimental Data</a><script data-card-contents-for-ri="1120502" type="text/json">{"id":1120502,"name":"Experimental Data","url":"https://www.academia.edu/Documents/in/Experimental_Data?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=22205436]'), work: {"id":22205436,"title":"An extended saturated liquid density equation","created_at":"2016-02-19T22:01:41.009-08:00","url":"https://www.academia.edu/22205436/An_extended_saturated_liquid_density_equation?f_ri=80799","dom_id":"work_22205436","summary":null,"downloadable_attachments":[{"id":42859686,"asset_id":22205436,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":35867874,"first_name":"Shahab","last_name":"Ayatollahi","domain_name":"sharif","page_name":"ShahabAyatollahi","display_name":"Shahab Ayatollahi","profile_url":"https://sharif.academia.edu/ShahabAyatollahi?f_ri=80799","photo":"https://0.academia-photos.com/35867874/11615910/12953230/s65_shahab.ayatollahi.jpg"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true},{"id":1120502,"name":"Experimental Data","url":"https://www.academia.edu/Documents/in/Experimental_Data?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_20571347" data-work_id="20571347" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/20571347/A_novel_approach_to_the_acoustic_characterisation_of_porous_road_surfaces">A novel approach to the acoustic characterisation of porous road surfaces</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Porous road surfaces offer an effective means of reducing the generation and propagation of noise from road traffic. However, the porosity of these surfaces can deteriorate over time, leading to a reduction in their noise reducing... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_20571347" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Porous road surfaces offer an effective means of reducing the generation and propagation of noise from road traffic. However, the porosity of these surfaces can deteriorate over time, leading to a reduction in their noise reducing properties. Efficient methods are therefore required for monitoring this performance. Existing techniques for performing in-situ measurements of acoustic absorption are unsuitable for use within the traffic stream. Static measurements using time domain Maximum Length Sequence (MLS) based techniques have been demonstrated to offer advantages over traditional techniques, presenting the opportunity for measurements under dynamic conditions. This paper describes the design of a system for carrying out dynamic MLS-based measurements. Results are presented which demonstrate that stable dynamic measurements can be carried out at speeds of up to 30 km/h.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/20571347" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="11808f346d20465352a979f268e001d6" rel="nofollow" data-download="{"attachment_id":41443539,"asset_id":20571347,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/41443539/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="41925355" href="https://bradford.academia.edu/GregWatts">Greg Watts</a><script data-card-contents-for-user="41925355" type="text/json">{"id":41925355,"first_name":"Greg","last_name":"Watts","domain_name":"bradford","page_name":"GregWatts","display_name":"Greg Watts","profile_url":"https://bradford.academia.edu/GregWatts?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_20571347 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="20571347"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 20571347, container: ".js-paper-rank-work_20571347", }); 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$(".js-view-count[data-work-id=20571347]").text(description); $(".js-view-count-work_20571347").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_20571347").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="20571347"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">7</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a>, <script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="841223" rel="nofollow" href="https://www.academia.edu/Documents/in/Road_Traffic">Road Traffic</a><script data-card-contents-for-ri="841223" type="text/json">{"id":841223,"name":"Road Traffic","url":"https://www.academia.edu/Documents/in/Road_Traffic?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=20571347]'), work: {"id":20571347,"title":"A novel approach to the acoustic characterisation of porous road surfaces","created_at":"2016-01-22T12:02:26.539-08:00","url":"https://www.academia.edu/20571347/A_novel_approach_to_the_acoustic_characterisation_of_porous_road_surfaces?f_ri=80799","dom_id":"work_20571347","summary":"Porous road surfaces offer an effective means of reducing the generation and propagation of noise from road traffic. However, the porosity of these surfaces can deteriorate over time, leading to a reduction in their noise reducing properties. Efficient methods are therefore required for monitoring this performance. Existing techniques for performing in-situ measurements of acoustic absorption are unsuitable for use within the traffic stream. Static measurements using time domain Maximum Length Sequence (MLS) based techniques have been demonstrated to offer advantages over traditional techniques, presenting the opportunity for measurements under dynamic conditions. This paper describes the design of a system for carrying out dynamic MLS-based measurements. Results are presented which demonstrate that stable dynamic measurements can be carried out at speeds of up to 30 km/h.","downloadable_attachments":[{"id":41443539,"asset_id":20571347,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":41925355,"first_name":"Greg","last_name":"Watts","domain_name":"bradford","page_name":"GregWatts","display_name":"Greg Watts","profile_url":"https://bradford.academia.edu/GregWatts?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":841223,"name":"Road Traffic","url":"https://www.academia.edu/Documents/in/Road_Traffic?f_ri=80799","nofollow":true},{"id":991005,"name":"Time Domain","url":"https://www.academia.edu/Documents/in/Time_Domain?f_ri=80799"},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799"},{"id":2255881,"name":"(Maximum Length Sequence","url":"https://www.academia.edu/Documents/in/_Maximum_Length_Sequence?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_19233944" data-work_id="19233944" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/19233944/High_contrast_ion_acceleration_at_intensities_exceeding_10_sup_21_Wcm_sup_2_">High contrast ion acceleration at intensities exceeding 10[sup 21] Wcm[sup −2]</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Ion acceleration from short pulse laser interactions at intensities of 2 Â 10 21 Wcm À2 was studied experimentally under a wide variety of parameters, including laser contrast, incidence angle, and target thickness. Trends in maximum... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_19233944" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Ion acceleration from short pulse laser interactions at intensities of 2 Â 10 21 Wcm À2 was studied experimentally under a wide variety of parameters, including laser contrast, incidence angle, and target thickness. Trends in maximum proton energy were observed, as well as evidence of improvement in the acceleration gradients by using dual plasma mirrors over traditional pulse cleaning techniques. Extremely high efficiency acceleration gradients were produced, accelerating both the contaminant layer and high charge state ions from the bulk of the target. Two dimensional particle-in-cell simulations enabled the study of the influence of scale length on submicron targets, where hydrodynamic expansion affects the rear surface as well as the front. Experimental evidence of larger electric fields for sharp density plasmas is observed in simulation results as well for such targets, where target ions are accelerated without the need for contaminant removal. V C 2013 AIP Publishing LLC. [http://dx.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/19233944" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="f2bae8e4a28e978e3f6a28af06530f2e" rel="nofollow" data-download="{"attachment_id":40506628,"asset_id":19233944,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/40506628/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39467753" href="https://independent.academia.edu/VictorYanovsky">Victor Yanovsky</a><script data-card-contents-for-user="39467753" type="text/json">{"id":39467753,"first_name":"Victor","last_name":"Yanovsky","domain_name":"independent","page_name":"VictorYanovsky","display_name":"Victor Yanovsky","profile_url":"https://independent.academia.edu/VictorYanovsky?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_19233944 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="19233944"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 19233944, container: ".js-paper-rank-work_19233944", }); });</script></li><li class="js-percentile-work_19233944 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 19233944; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_19233944"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_19233944 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="19233944"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 19233944; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=19233944]").text(description); $(".js-view-count-work_19233944").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_19233944").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="19233944"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=19233944]'), work: {"id":19233944,"title":"High contrast ion acceleration at intensities exceeding 10[sup 21] Wcm[sup −2]","created_at":"2015-11-30T07:15:17.291-08:00","url":"https://www.academia.edu/19233944/High_contrast_ion_acceleration_at_intensities_exceeding_10_sup_21_Wcm_sup_2_?f_ri=80799","dom_id":"work_19233944","summary":"Ion acceleration from short pulse laser interactions at intensities of 2 Â 10 21 Wcm À2 was studied experimentally under a wide variety of parameters, including laser contrast, incidence angle, and target thickness. Trends in maximum proton energy were observed, as well as evidence of improvement in the acceleration gradients by using dual plasma mirrors over traditional pulse cleaning techniques. Extremely high efficiency acceleration gradients were produced, accelerating both the contaminant layer and high charge state ions from the bulk of the target. Two dimensional particle-in-cell simulations enabled the study of the influence of scale length on submicron targets, where hydrodynamic expansion affects the rear surface as well as the front. Experimental evidence of larger electric fields for sharp density plasmas is observed in simulation results as well for such targets, where target ions are accelerated without the need for contaminant removal. V C 2013 AIP Publishing LLC. [http://dx.","downloadable_attachments":[{"id":40506628,"asset_id":19233944,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39467753,"first_name":"Victor","last_name":"Yanovsky","domain_name":"independent","page_name":"VictorYanovsky","display_name":"Victor Yanovsky","profile_url":"https://independent.academia.edu/VictorYanovsky?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_81641394" data-work_id="81641394" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/81641394/Photopyroelectric_Technique_for_Hemoglobin_Assessment_in_Human_Blood">Photopyroelectric Technique for Hemoglobin Assessment in Human Blood</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A new photopyroelectric (PPE) methodology, for optical characterization of general liquids, was used for the assessment of hemoglobin in human blood. The optical absorption coefficient of a hemoglobin reference was measured with this PPE... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_81641394" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A new photopyroelectric (PPE) methodology, for optical characterization of general liquids, was used for the assessment of hemoglobin in human blood. The optical absorption coefficient of a hemoglobin reference was measured with this PPE methodology and its corresponding absorptivity, at 532 nm, was obtained. This last reference was used for hemoglobin quantification of blood from a healthy man.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/81641394" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="8bb0899666c63ce14f7d568eefd021c6" rel="nofollow" data-download="{"attachment_id":87615629,"asset_id":81641394,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/87615629/download_file?st=MTc0MDIyMzU1Myw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13368295" href="https://independent.academia.edu/AbrahamBalderas">Abraham Balderas</a><script data-card-contents-for-user="13368295" type="text/json">{"id":13368295,"first_name":"Abraham","last_name":"Balderas","domain_name":"independent","page_name":"AbrahamBalderas","display_name":"Abraham Balderas","profile_url":"https://independent.academia.edu/AbrahamBalderas?f_ri=80799","photo":"https://0.academia-photos.com/13368295/5988822/6796041/s65_abraham.balderas.jpg_oh_18ff076dd8b0354ec35a2cc22fe0d2f5_oe_54d75760___gda___1423134719_0b375920acd67b6804776663da1554d9"}</script></span></span></li><li class="js-paper-rank-work_81641394 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="81641394"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 81641394, container: ".js-paper-rank-work_81641394", }); 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The optical absorption coefficient of a hemoglobin reference was measured with this PPE methodology and its corresponding absorptivity, at 532 nm, was obtained. This last reference was used for hemoglobin quantification of blood from a healthy man.","downloadable_attachments":[{"id":87615629,"asset_id":81641394,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13368295,"first_name":"Abraham","last_name":"Balderas","domain_name":"independent","page_name":"AbrahamBalderas","display_name":"Abraham Balderas","profile_url":"https://independent.academia.edu/AbrahamBalderas?f_ri=80799","photo":"https://0.academia-photos.com/13368295/5988822/6796041/s65_abraham.balderas.jpg_oh_18ff076dd8b0354ec35a2cc22fe0d2f5_oe_54d75760___gda___1423134719_0b375920acd67b6804776663da1554d9"}],"research_interests":[{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":846269,"name":"Thermophysics","url":"https://www.academia.edu/Documents/in/Thermophysics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_81418270" data-work_id="81418270" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/81418270/Measurements_of_activity_coefficient_at_infinite_dilution_for_organic_solutes_in_tetramethylammonium_chloride_ethylene_glycol_deep_eutectic_solvent_using_gas_liquid_chromatography">Measurements of activity coefficient at infinite dilution for organic solutes in tetramethylammonium chloride + ethylene glycol deep eutectic solvent using gas-liquid chromatography</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Deep eutectic solvents (DESs) are considered as the new ionic liquids (ILs) analogues that have emerged as potential alternative 'green' solvents, for a diversity of applications. In this study, a type III DES based on ammonium salt was... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_81418270" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Deep eutectic solvents (DESs) are considered as the new ionic liquids (ILs) analogues that have emerged as potential alternative 'green' solvents, for a diversity of applications. In this study, a type III DES based on ammonium salt was investigated as an alternative solvent to currently employed conventional organic solvents in separation processes. Activity coefficients at infinite dilution, g ∞ 13 for 19 organic solutes in the tetramethylammonium chloride þ ethylene glycol DES were measured by the gas-liquid chromatography (GLC) method at four temperatures in the range from (313.15e343.15) K. Experimental measurements were undertaken with an overall uncertainty of ±5.4%. The effect of the structure of the solutes on g ∞ 13 was also investigated. For all investigated solutes, Gibbs helmholtz relationship was utilised to derive partial molar excess enthalpy values at infinite dilution (DH E;ð∞Þ i) from experimental limiting activity coefficient data. From selectivity (S ∞ ij) and capacity (k ∞ j) values at infinte dilution, it was concluded that the investigated DES has the potential to replace a number of industrial solvents for the separation of various industrial mixtures.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/81418270" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="0dc23794746e253908bab49214557356" rel="nofollow" data-download="{"attachment_id":87467796,"asset_id":81418270,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/87467796/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="34172306" href="https://independent.academia.edu/KANIKITUMBA">KANIKI TUMBA</a><script data-card-contents-for-user="34172306" type="text/json">{"id":34172306,"first_name":"KANIKI","last_name":"TUMBA","domain_name":"independent","page_name":"KANIKITUMBA","display_name":"KANIKI TUMBA","profile_url":"https://independent.academia.edu/KANIKITUMBA?f_ri=80799","photo":"https://0.academia-photos.com/34172306/12724747/14153170/s65_kaniki.tumba.jpg"}</script></span></span></li><li class="js-paper-rank-work_81418270 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="81418270"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 81418270, container: ".js-paper-rank-work_81418270", }); 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$(".js-view-count[data-work-id=81418270]").text(description); $(".js-view-count-work_81418270").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_81418270").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="81418270"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="523" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemistry">Chemistry</a>, <script data-card-contents-for-ri="523" type="text/json">{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="629119" rel="nofollow" href="https://www.academia.edu/Documents/in/Fluid_phase_equilibria">Fluid phase equilibria</a><script data-card-contents-for-ri="629119" type="text/json">{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=81418270]'), work: {"id":81418270,"title":"Measurements of activity coefficient at infinite dilution for organic solutes in tetramethylammonium chloride + ethylene glycol deep eutectic solvent using gas-liquid chromatography","created_at":"2022-06-13T14:39:05.539-07:00","url":"https://www.academia.edu/81418270/Measurements_of_activity_coefficient_at_infinite_dilution_for_organic_solutes_in_tetramethylammonium_chloride_ethylene_glycol_deep_eutectic_solvent_using_gas_liquid_chromatography?f_ri=80799","dom_id":"work_81418270","summary":"Deep eutectic solvents (DESs) are considered as the new ionic liquids (ILs) analogues that have emerged as potential alternative 'green' solvents, for a diversity of applications. In this study, a type III DES based on ammonium salt was investigated as an alternative solvent to currently employed conventional organic solvents in separation processes. Activity coefficients at infinite dilution, g ∞ 13 for 19 organic solutes in the tetramethylammonium chloride þ ethylene glycol DES were measured by the gas-liquid chromatography (GLC) method at four temperatures in the range from (313.15e343.15) K. Experimental measurements were undertaken with an overall uncertainty of ±5.4%. The effect of the structure of the solutes on g ∞ 13 was also investigated. For all investigated solutes, Gibbs helmholtz relationship was utilised to derive partial molar excess enthalpy values at infinite dilution (DH E;ð∞Þ i) from experimental limiting activity coefficient data. From selectivity (S ∞ ij) and capacity (k ∞ j) values at infinte dilution, it was concluded that the investigated DES has the potential to replace a number of industrial solvents for the separation of various industrial mixtures.","downloadable_attachments":[{"id":87467796,"asset_id":81418270,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":34172306,"first_name":"KANIKI","last_name":"TUMBA","domain_name":"independent","page_name":"KANIKITUMBA","display_name":"KANIKI TUMBA","profile_url":"https://independent.academia.edu/KANIKITUMBA?f_ri=80799","photo":"https://0.academia-photos.com/34172306/12724747/14153170/s65_kaniki.tumba.jpg"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_76954933" data-work_id="76954933" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/76954933/Surface_charges_and_J_H_Poynting_s_disquisitions_on_energy_transfer_in_electrical_circuits">Surface charges and J H Poynting’s disquisitions on energy transfer in electrical circuits</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In this paper we review the examples of J H Poynting (1884) on the transfer of electromagnetic energy in DC circuits. These examples were strongly criticized by O Heaviside (1887). Heaviside stated that Poynting had a misconception about... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_76954933" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In this paper we review the examples of J H Poynting (1884) on the transfer of electromagnetic energy in DC circuits. These examples were strongly criticized by O Heaviside (1887). Heaviside stated that Poynting had a misconception about the nature of the electric field in the vicinity of a wire through which a current flows. The historical review of this conflict and its resolution based on the consideration of electrical charges on the surface of the wires can be useful in the courses of electromagnetism or circuit theory.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/76954933" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="ffb6733ea1c3674fecd51b72d02c0e61" rel="nofollow" data-download="{"attachment_id":84491427,"asset_id":76954933,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/84491427/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="7098653" href="https://rosario.academia.edu/Reinaldowelti">Reinaldo welti</a><script data-card-contents-for-user="7098653" type="text/json">{"id":7098653,"first_name":"Reinaldo","last_name":"welti","domain_name":"rosario","page_name":"Reinaldowelti","display_name":"Reinaldo welti","profile_url":"https://rosario.academia.edu/Reinaldowelti?f_ri=80799","photo":"https://0.academia-photos.com/7098653/88186182/76878464/s65_reinaldo.welti.jpeg"}</script></span></span></li><li class="js-paper-rank-work_76954933 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="76954933"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 76954933, container: ".js-paper-rank-work_76954933", }); });</script></li><li class="js-percentile-work_76954933 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76954933; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_76954933"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_76954933 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="76954933"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76954933; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76954933]").text(description); $(".js-view-count-work_76954933").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_76954933").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="76954933"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="498" rel="nofollow" href="https://www.academia.edu/Documents/in/Physics">Physics</a>, <script data-card-contents-for-ri="498" type="text/json">{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=76954933]'), work: {"id":76954933,"title":"Surface charges and J H Poynting’s disquisitions on energy transfer in electrical circuits","created_at":"2022-04-19T06:40:18.753-07:00","url":"https://www.academia.edu/76954933/Surface_charges_and_J_H_Poynting_s_disquisitions_on_energy_transfer_in_electrical_circuits?f_ri=80799","dom_id":"work_76954933","summary":"In this paper we review the examples of J H Poynting (1884) on the transfer of electromagnetic energy in DC circuits. These examples were strongly criticized by O Heaviside (1887). Heaviside stated that Poynting had a misconception about the nature of the electric field in the vicinity of a wire through which a current flows. The historical review of this conflict and its resolution based on the consideration of electrical charges on the surface of the wires can be useful in the courses of electromagnetism or circuit theory.","downloadable_attachments":[{"id":84491427,"asset_id":76954933,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":7098653,"first_name":"Reinaldo","last_name":"welti","domain_name":"rosario","page_name":"Reinaldowelti","display_name":"Reinaldo welti","profile_url":"https://rosario.academia.edu/Reinaldowelti?f_ri=80799","photo":"https://0.academia-photos.com/7098653/88186182/76878464/s65_reinaldo.welti.jpeg"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_76378356" data-work_id="76378356" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/76378356/Equations_of_state_for_hydrogen_bonding_systems">Equations of state for hydrogen bonding systems</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Considerable progress has been made over the last two decades in the modeling of hydrogen bonding fluids. Traditionally, the properties of hydrogen bonding solutions have been predicted and correlated using lattice models to give activity... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_76378356" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Considerable progress has been made over the last two decades in the modeling of hydrogen bonding fluids. Traditionally, the properties of hydrogen bonding solutions have been predicted and correlated using lattice models to give activity coefficients. Recently, several equations of state have been developed which can be used to predict activities and other configurational properties. This paper presents an overview of the specific types of chemical interactions that can be treated, the mathematical methods used to treat hydrogen bonding, and the similarities and differences in the underlying equations of state that are used to treat the "van der Waals" repulsive and attractive forces. Comparisons are made between chemical theories, quasichemical theories, and perturbation theories, including discussions on APACT, Panayiotou-Sanchez-Lacombe, and the SAFT equation.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/76378356" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="54f86f8eb8d22ac29a18079dd329571c" rel="nofollow" data-download="{"attachment_id":84105504,"asset_id":76378356,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/84105504/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="43509666" href="https://johnshopkins.academia.edu/MDonohue">Marc Donohue</a><script data-card-contents-for-user="43509666" type="text/json">{"id":43509666,"first_name":"Marc","last_name":"Donohue","domain_name":"johnshopkins","page_name":"MDonohue","display_name":"Marc Donohue","profile_url":"https://johnshopkins.academia.edu/MDonohue?f_ri=80799","photo":"https://0.academia-photos.com/43509666/44366345/34950297/s65_marc.donohue.jpg"}</script></span></span></li><li class="js-paper-rank-work_76378356 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="76378356"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 76378356, container: ".js-paper-rank-work_76378356", }); });</script></li><li class="js-percentile-work_76378356 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76378356; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_76378356"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_76378356 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="76378356"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76378356; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76378356]").text(description); $(".js-view-count-work_76378356").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_76378356").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="76378356"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">8</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="95016" rel="nofollow" href="https://www.academia.edu/Documents/in/Lattice_Beam_Model">Lattice Beam Model</a>, <script data-card-contents-for-ri="95016" type="text/json">{"id":95016,"name":"Lattice Beam Model","url":"https://www.academia.edu/Documents/in/Lattice_Beam_Model?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="212517" rel="nofollow" href="https://www.academia.edu/Documents/in/Van_Der_Waals">Van Der Waals</a><script data-card-contents-for-ri="212517" type="text/json">{"id":212517,"name":"Van Der Waals","url":"https://www.academia.edu/Documents/in/Van_Der_Waals?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=76378356]'), work: {"id":76378356,"title":"Equations of state for hydrogen bonding systems","created_at":"2022-04-13T21:01:20.512-07:00","url":"https://www.academia.edu/76378356/Equations_of_state_for_hydrogen_bonding_systems?f_ri=80799","dom_id":"work_76378356","summary":"Considerable progress has been made over the last two decades in the modeling of hydrogen bonding fluids. Traditionally, the properties of hydrogen bonding solutions have been predicted and correlated using lattice models to give activity coefficients. Recently, several equations of state have been developed which can be used to predict activities and other configurational properties. This paper presents an overview of the specific types of chemical interactions that can be treated, the mathematical methods used to treat hydrogen bonding, and the similarities and differences in the underlying equations of state that are used to treat the \"van der Waals\" repulsive and attractive forces. Comparisons are made between chemical theories, quasichemical theories, and perturbation theories, including discussions on APACT, Panayiotou-Sanchez-Lacombe, and the SAFT equation.","downloadable_attachments":[{"id":84105504,"asset_id":76378356,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":43509666,"first_name":"Marc","last_name":"Donohue","domain_name":"johnshopkins","page_name":"MDonohue","display_name":"Marc Donohue","profile_url":"https://johnshopkins.academia.edu/MDonohue?f_ri=80799","photo":"https://0.academia-photos.com/43509666/44366345/34950297/s65_marc.donohue.jpg"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":95016,"name":"Lattice Beam Model","url":"https://www.academia.edu/Documents/in/Lattice_Beam_Model?f_ri=80799","nofollow":true},{"id":212517,"name":"Van Der Waals","url":"https://www.academia.edu/Documents/in/Van_Der_Waals?f_ri=80799","nofollow":true},{"id":240148,"name":"Hydrogen Bond","url":"https://www.academia.edu/Documents/in/Hydrogen_Bond?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"},{"id":1320599,"name":"Equation of State","url":"https://www.academia.edu/Documents/in/Equation_of_State?f_ri=80799"},{"id":1600931,"name":"Perturbation Theory","url":"https://www.academia.edu/Documents/in/Perturbation_Theory?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_73924969" data-work_id="73924969" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/73924969/Microcomputer_based_singing_ability_assessment_and_development">Microcomputer-based singing ability assessment and development</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A new mwrocomputer-based system ts descrtbed whtch has been developed for the assessment and development of smgmg abthty lt makes use of a spectally developed hardware interface whwh esttmates the fundamental frequency of a sung or spoken... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_73924969" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A new mwrocomputer-based system ts descrtbed whtch has been developed for the assessment and development of smgmg abthty lt makes use of a spectally developed hardware interface whwh esttmates the fundamental frequency of a sung or spoken mput as the basts for (a) a measurement of vocal pttchmg accuracy (assessment), and (b) a vocal pttch &splay to provtde msual feedback (development) Results are dtscussed whwh are based on a study carrted out wtth the syatem in a Brtttsh prtmary school, and they mdtcate that this system ts effecttve m promotmg singing development</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/73924969" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="6735b217cbe44e0fc1e9fbe73cebd3b3" rel="nofollow" data-download="{"attachment_id":82264377,"asset_id":73924969,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/82264377/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="5650800" href="https://pprlgroup.academia.edu/DavidHoward">David Howard</a><script data-card-contents-for-user="5650800" type="text/json">{"id":5650800,"first_name":"David","last_name":"Howard","domain_name":"pprlgroup","page_name":"DavidHoward","display_name":"David Howard","profile_url":"https://pprlgroup.academia.edu/DavidHoward?f_ri=80799","photo":"https://0.academia-photos.com/5650800/12566594/13981587/s65_david.howard.jpg"}</script></span></span></li><li class="js-paper-rank-work_73924969 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="73924969"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 73924969, container: ".js-paper-rank-work_73924969", }); });</script></li><li class="js-percentile-work_73924969 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 73924969; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_73924969"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_73924969 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="73924969"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 73924969; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=73924969]").text(description); $(".js-view-count-work_73924969").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_73924969").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="73924969"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a>, <script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1280929" rel="nofollow" href="https://www.academia.edu/Documents/in/Applied_Acoustics">Applied Acoustics</a><script data-card-contents-for-ri="1280929" type="text/json">{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=73924969]'), work: {"id":73924969,"title":"Microcomputer-based singing ability assessment and development","created_at":"2022-03-16T23:23:03.829-07:00","url":"https://www.academia.edu/73924969/Microcomputer_based_singing_ability_assessment_and_development?f_ri=80799","dom_id":"work_73924969","summary":"A new mwrocomputer-based system ts descrtbed whtch has been developed for the assessment and development of smgmg abthty lt makes use of a spectally developed hardware interface whwh esttmates the fundamental frequency of a sung or spoken mput as the basts for (a) a measurement of vocal pttchmg accuracy (assessment), and (b) a vocal pttch \u0026splay to provtde msual feedback (development) Results are dtscussed whwh are based on a study carrted out wtth the syatem in a Brtttsh prtmary school, and they mdtcate that this system ts effecttve m promotmg singing development","downloadable_attachments":[{"id":82264377,"asset_id":73924969,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":5650800,"first_name":"David","last_name":"Howard","domain_name":"pprlgroup","page_name":"DavidHoward","display_name":"David Howard","profile_url":"https://pprlgroup.academia.edu/DavidHoward?f_ri=80799","photo":"https://0.academia-photos.com/5650800/12566594/13981587/s65_david.howard.jpg"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_61424944" data-work_id="61424944" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/61424944/Laser_driven_cylindrical_compression_of_targets_for_fast_electron_transport_study_in_warm_and_dense_plasmas">Laser-driven cylindrical compression of targets for fast electron transport study in warm and dense plasmas</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Fast ignition requires a precise knowledge of fast electron propagation in a dense hydrogen plasma. In this context, a dedicated HiPER (High Power laser Energy Research) experiment was performed on the VULCAN laser facility where the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_61424944" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Fast ignition requires a precise knowledge of fast electron propagation in a dense hydrogen plasma. In this context, a dedicated HiPER (High Power laser Energy Research) experiment was performed on the VULCAN laser facility where the propagation of relativistic electron beams through cylindrically compressed plastic targets was studied. In this paper, we characterize the plasma parameters such as temperature and density during the compression of cylindrical polyimide shells filled with CH foams at three different initial densities. X-ray and proton radiography were used to measure the cylinder radius at different stages of the compression. By comparing both diagnostics results with 2D hydrodynamic simulations, we could infer densities from 2 to 11 g=cm 3 and temperatures from 30 to 120 eV at maximum compression at the center of targets. According to the initial foam density, kinetic, coupled (sometimes degenerated) plasmas were obtained. The temporal and spatial evolution of the resulting areal densities and electrical conductivities allow for testing electron transport in a wide range of configurations. V</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/61424944" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5df3fe7ca6ca33e023d70e7c76779ba3" rel="nofollow" data-download="{"attachment_id":74458097,"asset_id":61424944,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/74458097/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="104153760" href="https://independent.academia.edu/RashidaJafer">Rashida Jafer</a><script data-card-contents-for-user="104153760" type="text/json">{"id":104153760,"first_name":"Rashida","last_name":"Jafer","domain_name":"independent","page_name":"RashidaJafer","display_name":"Rashida Jafer","profile_url":"https://independent.academia.edu/RashidaJafer?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_61424944 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="61424944"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 61424944, container: ".js-paper-rank-work_61424944", }); });</script></li><li class="js-percentile-work_61424944 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 61424944; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_61424944"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_61424944 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="61424944"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 61424944; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=61424944]").text(description); $(".js-view-count-work_61424944").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_61424944").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="61424944"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">17</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="4987" rel="nofollow" href="https://www.academia.edu/Documents/in/Kinetics">Kinetics</a>, <script data-card-contents-for-ri="4987" type="text/json">{"id":4987,"name":"Kinetics","url":"https://www.academia.edu/Documents/in/Kinetics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="16012" rel="nofollow" href="https://www.academia.edu/Documents/in/High_Energy_Density_Physics">High Energy Density Physics</a>, <script data-card-contents-for-ri="16012" type="text/json">{"id":16012,"name":"High Energy Density Physics","url":"https://www.academia.edu/Documents/in/High_Energy_Density_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="20949" rel="nofollow" href="https://www.academia.edu/Documents/in/Laser_Plasma_Interactions">Laser Plasma Interactions</a>, <script data-card-contents-for-ri="20949" type="text/json">{"id":20949,"name":"Laser Plasma Interactions","url":"https://www.academia.edu/Documents/in/Laser_Plasma_Interactions?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="33315" rel="nofollow" href="https://www.academia.edu/Documents/in/Inertial_Fusion_Energy">Inertial Fusion Energy</a><script data-card-contents-for-ri="33315" type="text/json">{"id":33315,"name":"Inertial Fusion Energy","url":"https://www.academia.edu/Documents/in/Inertial_Fusion_Energy?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=61424944]'), work: {"id":61424944,"title":"Laser-driven cylindrical compression of targets for fast electron transport study in warm and dense plasmas","created_at":"2021-11-09T13:03:41.912-08:00","url":"https://www.academia.edu/61424944/Laser_driven_cylindrical_compression_of_targets_for_fast_electron_transport_study_in_warm_and_dense_plasmas?f_ri=80799","dom_id":"work_61424944","summary":"Fast ignition requires a precise knowledge of fast electron propagation in a dense hydrogen plasma. In this context, a dedicated HiPER (High Power laser Energy Research) experiment was performed on the VULCAN laser facility where the propagation of relativistic electron beams through cylindrically compressed plastic targets was studied. In this paper, we characterize the plasma parameters such as temperature and density during the compression of cylindrical polyimide shells filled with CH foams at three different initial densities. X-ray and proton radiography were used to measure the cylinder radius at different stages of the compression. By comparing both diagnostics results with 2D hydrodynamic simulations, we could infer densities from 2 to 11 g=cm 3 and temperatures from 30 to 120 eV at maximum compression at the center of targets. According to the initial foam density, kinetic, coupled (sometimes degenerated) plasmas were obtained. The temporal and spatial evolution of the resulting areal densities and electrical conductivities allow for testing electron transport in a wide range of configurations. V","downloadable_attachments":[{"id":74458097,"asset_id":61424944,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":104153760,"first_name":"Rashida","last_name":"Jafer","domain_name":"independent","page_name":"RashidaJafer","display_name":"Rashida Jafer","profile_url":"https://independent.academia.edu/RashidaJafer?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":4987,"name":"Kinetics","url":"https://www.academia.edu/Documents/in/Kinetics?f_ri=80799","nofollow":true},{"id":16012,"name":"High Energy Density Physics","url":"https://www.academia.edu/Documents/in/High_Energy_Density_Physics?f_ri=80799","nofollow":true},{"id":20949,"name":"Laser Plasma Interactions","url":"https://www.academia.edu/Documents/in/Laser_Plasma_Interactions?f_ri=80799","nofollow":true},{"id":33315,"name":"Inertial Fusion Energy","url":"https://www.academia.edu/Documents/in/Inertial_Fusion_Energy?f_ri=80799","nofollow":true},{"id":56001,"name":"X Rays","url":"https://www.academia.edu/Documents/in/X_Rays?f_ri=80799"},{"id":60653,"name":"Transport Properties","url":"https://www.academia.edu/Documents/in/Transport_Properties?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":186094,"name":"Electron Transport","url":"https://www.academia.edu/Documents/in/Electron_Transport?f_ri=80799"},{"id":323552,"name":"High Power","url":"https://www.academia.edu/Documents/in/High_Power?f_ri=80799"},{"id":436755,"name":"Degeneration","url":"https://www.academia.edu/Documents/in/Degeneration?f_ri=80799"},{"id":506413,"name":"Laser Matter Interactions","url":"https://www.academia.edu/Documents/in/Laser_Matter_Interactions?f_ri=80799"},{"id":882075,"name":"Light Propagation","url":"https://www.academia.edu/Documents/in/Light_Propagation?f_ri=80799"},{"id":912885,"name":"Gamma Ray","url":"https://www.academia.edu/Documents/in/Gamma_Ray?f_ri=80799"},{"id":920313,"name":"Electron Beam","url":"https://www.academia.edu/Documents/in/Electron_Beam?f_ri=80799"},{"id":1202042,"name":"Electric Conductivity","url":"https://www.academia.edu/Documents/in/Electric_Conductivity?f_ri=80799"},{"id":1753694,"name":"Plasma Diagnostic","url":"https://www.academia.edu/Documents/in/Plasma_Diagnostic?f_ri=80799"},{"id":2756779,"name":"transport process","url":"https://www.academia.edu/Documents/in/transport_process?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_60124226" data-work_id="60124226" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/60124226/Dendritic_flux_avalanches_in_superconducting_Nb3Sn_films">Dendritic flux avalanches in superconducting Nb3Sn films</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The penetration of magnetic flux into a thin superconducting film of Nb 3 Sn with critical temperature 17.8 K and critical current density 6 MA/cm 2 was visualized using magneto-optical imaging. Below 8 K an avalanche-like flux... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_60124226" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The penetration of magnetic flux into a thin superconducting film of Nb 3 Sn with critical temperature 17.8 K and critical current density 6 MA/cm 2 was visualized using magneto-optical imaging. Below 8 K an avalanche-like flux penetration in form of big and branching dendritic structures was observed in response to increasing perpendicular applied field. When a growing dendritic branch meets a linear defect in the film, several scenarios were observed: the branch can turn and propagate along the defect, continue propagation right through it, or ''tunnel'' along a flux-filled defect and continue growth from its other end. The avalanches manifest themselves in numerous small and random jumps found in the magnetization curve.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/60124226" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="8fd384009d2a7d7ec60724f9de41646e" rel="nofollow" data-download="{"attachment_id":73703210,"asset_id":60124226,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/73703210/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="72428639" href="https://independent.academia.edu/YGalperin">Yuri Galperin</a><script data-card-contents-for-user="72428639" type="text/json">{"id":72428639,"first_name":"Yuri","last_name":"Galperin","domain_name":"independent","page_name":"YGalperin","display_name":"Yuri Galperin","profile_url":"https://independent.academia.edu/YGalperin?f_ri=80799","photo":"https://0.academia-photos.com/72428639/18559050/18526911/s65_yuri.galperin.jpg"}</script></span></span></li><li class="js-paper-rank-work_60124226 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="60124226"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 60124226, container: ".js-paper-rank-work_60124226", }); 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Below 8 K an avalanche-like flux penetration in form of big and branching dendritic structures was observed in response to increasing perpendicular applied field. When a growing dendritic branch meets a linear defect in the film, several scenarios were observed: the branch can turn and propagate along the defect, continue propagation right through it, or ''tunnel'' along a flux-filled defect and continue growth from its other end. The avalanches manifest themselves in numerous small and random jumps found in the magnetization curve.","downloadable_attachments":[{"id":73703210,"asset_id":60124226,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":72428639,"first_name":"Yuri","last_name":"Galperin","domain_name":"independent","page_name":"YGalperin","display_name":"Yuri Galperin","profile_url":"https://independent.academia.edu/YGalperin?f_ri=80799","photo":"https://0.academia-photos.com/72428639/18559050/18526911/s65_yuri.galperin.jpg"}],"research_interests":[{"id":506,"name":"Cryogenics","url":"https://www.academia.edu/Documents/in/Cryogenics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":101573,"name":"Thin Film","url":"https://www.academia.edu/Documents/in/Thin_Film?f_ri=80799","nofollow":true},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering?f_ri=80799","nofollow":true},{"id":1394433,"name":"Critical Temperature","url":"https://www.academia.edu/Documents/in/Critical_Temperature?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_47563086" data-work_id="47563086" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/47563086/Implementation_of_active_noise_control_in_a_multi_modal_spray_dryer_exhaust_stack">Implementation of active noise control in a multi-modal spray dryer exhaust stack</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Tonal noise emitted from large-diameter spray dryer exhaust stacks used in the dairy industry can give rise to complaints from nearby communities. In many cases, the tone at the fan blade passing frequency is characterized by a frequency... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47563086" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Tonal noise emitted from large-diameter spray dryer exhaust stacks used in the dairy industry can give rise to complaints from nearby communities. In many cases, the tone at the fan blade passing frequency is characterized by a frequency above the first mode cut on frequency of the exhaust stack and both its amplitude and the frequency are time varying. The variation in amplitude is a result of turbulence and temperature variations in the duct which cause angular variations in the nodal plane of modes with diametrical nodes. This in turn results in large fluctuations in sound pressure with time at any specified location in the duct, thus presenting a significant challenge for an ANC system with fixed control source and error sensor locations. In many food processing industries, the use of sound absorptive materials in silencers is not acceptable and, particularly when the fan speed is variable, it is difficult to achieve an acceptable passive solution at a reasonable cost. Here, the design and implementation of an active noise control system for tonal noise propagating above the cut-on frequency of the first higher order mode in large size cylindrical industrial exhaust stack is discussed, where the frequency and amplitude vary significantly and relatively rapidly with time. Physical system design principles and control algorithm optimization for a practical active noise control system are 0003-682X/$ -see front matter Ó .au (X. 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In many cases, the tone at the fan blade passing frequency is characterized by a frequency above the first mode cut on frequency of the exhaust stack and both its amplitude and the frequency are time varying. The variation in amplitude is a result of turbulence and temperature variations in the duct which cause angular variations in the nodal plane of modes with diametrical nodes. This in turn results in large fluctuations in sound pressure with time at any specified location in the duct, thus presenting a significant challenge for an ANC system with fixed control source and error sensor locations. In many food processing industries, the use of sound absorptive materials in silencers is not acceptable and, particularly when the fan speed is variable, it is difficult to achieve an acceptable passive solution at a reasonable cost. Here, the design and implementation of an active noise control system for tonal noise propagating above the cut-on frequency of the first higher order mode in large size cylindrical industrial exhaust stack is discussed, where the frequency and amplitude vary significantly and relatively rapidly with time. Physical system design principles and control algorithm optimization for a practical active noise control system are 0003-682X/$ -see front matter Ó .au (X. Li).","downloadable_attachments":[{"id":66591849,"asset_id":47563086,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":187698979,"first_name":"Colin","last_name":"Hansen","domain_name":"independent","page_name":"ColinHansen2","display_name":"Colin Hansen","profile_url":"https://independent.academia.edu/ColinHansen2?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div 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Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=46833825]'), work: {"id":46833825,"title":"Experimental research on structure-borne noise at pulse-width-modulation excitation","created_at":"2021-04-13T11:38:26.429-07:00","url":"https://www.academia.edu/46833825/Experimental_research_on_structure_borne_noise_at_pulse_width_modulation_excitation?f_ri=80799","dom_id":"work_46833825","summary":null,"downloadable_attachments":[],"ordered_authors":[{"id":51541481,"first_name":"Janez","last_name":"Luznar","domain_name":"independent","page_name":"JanezLuznar","display_name":"Janez Luznar","profile_url":"https://independent.academia.edu/JanezLuznar?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":211489510,"first_name":"Janko","last_name":"Slavič","domain_name":"independent","page_name":"JankoSlavič","display_name":"Janko Slavič","profile_url":"https://independent.academia.edu/JankoSlavi%C4%8D?f_ri=80799","photo":"https://gravatar.com/avatar/28ca217ea2ae2b281dfe05c10cbaaf60?s=65"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_27478727" data-work_id="27478727" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" rel="nofollow" href="https://www.academia.edu/27478727/Excess_properties_and_isobaric_vapor_liquid_equilibria_for_four_binary_systems_of_alkyl_methyl_to_butyl_methanoates_with_decane">Excess properties and isobaric vapor–liquid equilibria for four binary systems of alkyl (methyl to butyl) methanoates with decane</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This work shows the experimental data of excess properties at several temperatures and the vapor–liquid equilibria (VLE) obtained for four binary systems of alkyl methanoates (methyl to butyl) with decane, all measured at constant... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_27478727" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This work shows the experimental data of excess properties at several temperatures and the vapor–liquid equilibria (VLE) obtained for four binary systems of alkyl methanoates (methyl to butyl) with decane, all measured at constant pressure of 101.32kPa. The isobaric VLE data were thermodynamically consistent according to the Fredenslund test and did not present an azeotrope. The experimental data of HmE</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/27478727" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="50650727" href="https://feszaragoza.academia.edu/juanortega">juan ortega</a><script data-card-contents-for-user="50650727" type="text/json">{"id":50650727,"first_name":"juan","last_name":"ortega","domain_name":"feszaragoza","page_name":"juanortega","display_name":"juan ortega","profile_url":"https://feszaragoza.academia.edu/juanortega?f_ri=80799","photo":"https://0.academia-photos.com/50650727/31585409/28927650/s65_juan.ortega.jpg"}</script></span></span></li><li class="js-paper-rank-work_27478727 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="27478727"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 27478727, container: ".js-paper-rank-work_27478727", }); 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$(".js-view-count[data-work-id=27478727]").text(description); $(".js-view-count-work_27478727").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_27478727").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="27478727"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">15</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="522" rel="nofollow" href="https://www.academia.edu/Documents/in/Thermodynamics">Thermodynamics</a>, <script data-card-contents-for-ri="522" type="text/json">{"id":522,"name":"Thermodynamics","url":"https://www.academia.edu/Documents/in/Thermodynamics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="3586" rel="nofollow" href="https://www.academia.edu/Documents/in/VLE">VLE</a>, <script data-card-contents-for-ri="3586" type="text/json">{"id":3586,"name":"VLE","url":"https://www.academia.edu/Documents/in/VLE?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=27478727]'), work: {"id":27478727,"title":"Excess properties and isobaric vapor–liquid equilibria for four binary systems of alkyl (methyl to butyl) methanoates with decane","created_at":"2016-08-02T13:29:39.639-07:00","url":"https://www.academia.edu/27478727/Excess_properties_and_isobaric_vapor_liquid_equilibria_for_four_binary_systems_of_alkyl_methyl_to_butyl_methanoates_with_decane?f_ri=80799","dom_id":"work_27478727","summary":"This work shows the experimental data of excess properties at several temperatures and the vapor–liquid equilibria (VLE) obtained for four binary systems of alkyl methanoates (methyl to butyl) with decane, all measured at constant pressure of 101.32kPa. The isobaric VLE data were thermodynamically consistent according to the Fredenslund test and did not present an azeotrope. The experimental data of HmE","downloadable_attachments":[],"ordered_authors":[{"id":50650727,"first_name":"juan","last_name":"ortega","domain_name":"feszaragoza","page_name":"juanortega","display_name":"juan ortega","profile_url":"https://feszaragoza.academia.edu/juanortega?f_ri=80799","photo":"https://0.academia-photos.com/50650727/31585409/28927650/s65_juan.ortega.jpg"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":522,"name":"Thermodynamics","url":"https://www.academia.edu/Documents/in/Thermodynamics?f_ri=80799","nofollow":true},{"id":3586,"name":"VLE","url":"https://www.academia.edu/Documents/in/VLE?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":81504,"name":"Correlation","url":"https://www.academia.edu/Documents/in/Correlation?f_ri=80799"},{"id":114712,"name":"Enthalpy","url":"https://www.academia.edu/Documents/in/Enthalpy?f_ri=80799"},{"id":163342,"name":"Molar volume","url":"https://www.academia.edu/Documents/in/Molar_volume?f_ri=80799"},{"id":247487,"name":"Temperature Dependence","url":"https://www.academia.edu/Documents/in/Temperature_Dependence?f_ri=80799"},{"id":592549,"name":"Interaction effect","url":"https://www.academia.edu/Documents/in/Interaction_effect?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"},{"id":1114988,"name":"Vapor Liquid Equilibria","url":"https://www.academia.edu/Documents/in/Vapor_Liquid_Equilibria?f_ri=80799"},{"id":1120502,"name":"Experimental Data","url":"https://www.academia.edu/Documents/in/Experimental_Data?f_ri=80799"},{"id":2037336,"name":"Phase Equilibrium","url":"https://www.academia.edu/Documents/in/Phase_Equilibrium?f_ri=80799"},{"id":2413807,"name":"Generic model","url":"https://www.academia.edu/Documents/in/Generic_model?f_ri=80799"},{"id":2491136,"name":"Parametric Model","url":"https://www.academia.edu/Documents/in/Parametric_Model?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_12023209" data-work_id="12023209" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/12023209/Simple_and_inexpensive_cryogenic_bolometers">Simple and inexpensive cryogenic bolometers</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Simple and inexpensive low-temperature bolometers have been fabricated using commercial thick-film resistors. The bolometer resistance depends both on the temperature and on the bias voltage. The responsivity and time constant are deduced... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_12023209" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Simple and inexpensive low-temperature bolometers have been fabricated using commercial thick-film resistors. The bolometer resistance depends both on the temperature and on the bias voltage. The responsivity and time constant are deduced in this non-ideal case.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/12023209" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7d3eaa407142340758632fb0589408fa" rel="nofollow" data-download="{"attachment_id":46400283,"asset_id":12023209,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/46400283/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="29952364" href="https://independent.academia.edu/SilvanaTerreni">Silvana Terreni</a><script data-card-contents-for-user="29952364" type="text/json">{"id":29952364,"first_name":"Silvana","last_name":"Terreni","domain_name":"independent","page_name":"SilvanaTerreni","display_name":"Silvana Terreni","profile_url":"https://independent.academia.edu/SilvanaTerreni?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_12023209 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="12023209"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 12023209, container: ".js-paper-rank-work_12023209", }); 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$(".js-view-count[data-work-id=12023209]").text(description); $(".js-view-count-work_12023209").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_12023209").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="12023209"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="506" rel="nofollow" href="https://www.academia.edu/Documents/in/Cryogenics">Cryogenics</a>, <script data-card-contents-for-ri="506" type="text/json">{"id":506,"name":"Cryogenics","url":"https://www.academia.edu/Documents/in/Cryogenics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="554780" rel="nofollow" href="https://www.academia.edu/Documents/in/Interdisciplinary_Engineering">Interdisciplinary Engineering</a><script data-card-contents-for-ri="554780" type="text/json">{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=12023209]'), work: {"id":12023209,"title":"Simple and inexpensive cryogenic bolometers","created_at":"2015-04-20T05:04:05.332-07:00","url":"https://www.academia.edu/12023209/Simple_and_inexpensive_cryogenic_bolometers?f_ri=80799","dom_id":"work_12023209","summary":"Simple and inexpensive low-temperature bolometers have been fabricated using commercial thick-film resistors. The bolometer resistance depends both on the temperature and on the bias voltage. The responsivity and time constant are deduced in this non-ideal case.","downloadable_attachments":[{"id":46400283,"asset_id":12023209,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":29952364,"first_name":"Silvana","last_name":"Terreni","domain_name":"independent","page_name":"SilvanaTerreni","display_name":"Silvana Terreni","profile_url":"https://independent.academia.edu/SilvanaTerreni?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":506,"name":"Cryogenics","url":"https://www.academia.edu/Documents/in/Cryogenics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_20819464" data-work_id="20819464" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/20819464/Prediction_of_vapor_liquid_equilibrium_for_binary_systems_containing_HFEs_by_using_artificial_neural_network">Prediction of vapor–liquid equilibrium for binary systems containing HFEs by using artificial neural network</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A method using artificial neural network (ANN) was applied to estimate the vapor-liquid equilibrium (VLE) for the binary systems containing hydrofluoroethers (HFEs) and polar compounds. Our new estimation method is composed of three... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_20819464" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A method using artificial neural network (ANN) was applied to estimate the vapor-liquid equilibrium (VLE) for the binary systems containing hydrofluoroethers (HFEs) and polar compounds. Our new estimation method is composed of three steps. In the first step, the sign of logarithm of activity coefficient (γ ) is estimated for each binary system using ANN, because it had been found that the binary systems containing HFEs show different thermodynamic behaviors depending on the sign for ln(γ ). In the second step, two sets of relation between liquid mole fraction and ln(γ ) are constructed: one held for the case of positive sign and the other held for that of negative sign. In the third step, vapor-liquid composition and equilibrium temperature are calculated using the estimated activity coefficient. In order to construct this new method, the isobaric VLE data of 18 binary systems including HFEs was used. As a result, our new method could estimate VLE with reasonable accuracy.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/20819464" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="71eaaa07851636a95ebb5b0174a316f0" rel="nofollow" data-download="{"attachment_id":41579645,"asset_id":20819464,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/41579645/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="42113163" href="https://independent.academia.edu/TakadaAkira">Akira Takada</a><script data-card-contents-for-user="42113163" type="text/json">{"id":42113163,"first_name":"Akira","last_name":"Takada","domain_name":"independent","page_name":"TakadaAkira","display_name":"Akira Takada","profile_url":"https://independent.academia.edu/TakadaAkira?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_20819464 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="20819464"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 20819464, container: ".js-paper-rank-work_20819464", }); });</script></li><li class="js-percentile-work_20819464 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 20819464; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_20819464"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_20819464 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="20819464"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 20819464; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=20819464]").text(description); $(".js-view-count-work_20819464").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_20819464").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="20819464"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">11</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="522" rel="nofollow" href="https://www.academia.edu/Documents/in/Thermodynamics">Thermodynamics</a>, <script data-card-contents-for-ri="522" type="text/json">{"id":522,"name":"Thermodynamics","url":"https://www.academia.edu/Documents/in/Thermodynamics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="7968" rel="nofollow" href="https://www.academia.edu/Documents/in/Prediction">Prediction</a>, <script data-card-contents-for-ri="7968" type="text/json">{"id":7968,"name":"Prediction","url":"https://www.academia.edu/Documents/in/Prediction?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="26066" rel="nofollow" href="https://www.academia.edu/Documents/in/Neural_Network">Neural Network</a><script data-card-contents-for-ri="26066" type="text/json">{"id":26066,"name":"Neural Network","url":"https://www.academia.edu/Documents/in/Neural_Network?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=20819464]'), work: {"id":20819464,"title":"Prediction of vapor–liquid equilibrium for binary systems containing HFEs by using artificial neural network","created_at":"2016-01-26T00:12:18.762-08:00","url":"https://www.academia.edu/20819464/Prediction_of_vapor_liquid_equilibrium_for_binary_systems_containing_HFEs_by_using_artificial_neural_network?f_ri=80799","dom_id":"work_20819464","summary":"A method using artificial neural network (ANN) was applied to estimate the vapor-liquid equilibrium (VLE) for the binary systems containing hydrofluoroethers (HFEs) and polar compounds. Our new estimation method is composed of three steps. In the first step, the sign of logarithm of activity coefficient (γ ) is estimated for each binary system using ANN, because it had been found that the binary systems containing HFEs show different thermodynamic behaviors depending on the sign for ln(γ ). In the second step, two sets of relation between liquid mole fraction and ln(γ ) are constructed: one held for the case of positive sign and the other held for that of negative sign. In the third step, vapor-liquid composition and equilibrium temperature are calculated using the estimated activity coefficient. In order to construct this new method, the isobaric VLE data of 18 binary systems including HFEs was used. As a result, our new method could estimate VLE with reasonable accuracy.","downloadable_attachments":[{"id":41579645,"asset_id":20819464,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":42113163,"first_name":"Akira","last_name":"Takada","domain_name":"independent","page_name":"TakadaAkira","display_name":"Akira Takada","profile_url":"https://independent.academia.edu/TakadaAkira?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":522,"name":"Thermodynamics","url":"https://www.academia.edu/Documents/in/Thermodynamics?f_ri=80799","nofollow":true},{"id":7968,"name":"Prediction","url":"https://www.academia.edu/Documents/in/Prediction?f_ri=80799","nofollow":true},{"id":26066,"name":"Neural Network","url":"https://www.academia.edu/Documents/in/Neural_Network?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":264903,"name":"Vapor liquid equilibrium","url":"https://www.academia.edu/Documents/in/Vapor_liquid_equilibrium?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"},{"id":1137227,"name":"Activity Coefficient","url":"https://www.academia.edu/Documents/in/Activity_Coefficient?f_ri=80799"},{"id":1180343,"name":"Estimation Method","url":"https://www.academia.edu/Documents/in/Estimation_Method?f_ri=80799"},{"id":1211304,"name":"Artificial Neural Network","url":"https://www.academia.edu/Documents/in/Artificial_Neural_Network?f_ri=80799"},{"id":2037336,"name":"Phase Equilibrium","url":"https://www.academia.edu/Documents/in/Phase_Equilibrium?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_45027024" data-work_id="45027024" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/45027024/Multimedia_Presentation_of_Musical_Instruments">Multimedia Presentation of Musical Instruments</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The problem presented in the paper belongs to a wide subject concerning the use of multimedia technology for the improvement of educational activities in museums and for attracting the audience with objects of art. Several examples of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_45027024" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The problem presented in the paper belongs to a wide subject concerning the use of multimedia technology for the improvement of educational activities in museums and for attracting the audience with objects of art. Several examples of temporal and regular multimedia performances in galleries are known in Poland and abroad, but still the technology is not fully used in traditional museums. In the paper, the case study of multimedia presentation devoted to the collection of the historical instruments from the Museum of Musical Instruments in Poznań is described. By their nature, musical instruments are interactive, but for the reasons of security and costs, only on rare occasions may visitors listen to their sound. Multimedia can change this situation. The inspiration for creating the multimedia presentation was the 250th Anniversary of Wolfgang Amadeus Mozart birth. The historical 18th century instruments from the collection of the museum accompanied by the music of the composer have been virtually exposed. Shown during the "Museums Night" in May 2006, the presentation has gained interest of hundreds of guests and proved useful for future educational actions.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/45027024" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="cbb4cd6737f6239ff7be082b3c80d249" rel="nofollow" data-download="{"attachment_id":65576391,"asset_id":45027024,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/65576391/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="184487419" href="https://wats-kompozyty.academia.edu/Ewa%C5%81ukasik">Ewa Łukasik</a><script data-card-contents-for-user="184487419" type="text/json">{"id":184487419,"first_name":"Ewa","last_name":"Łukasik","domain_name":"wats-kompozyty","page_name":"EwaŁukasik","display_name":"Ewa Łukasik","profile_url":"https://wats-kompozyty.academia.edu/Ewa%C5%81ukasik?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_45027024 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="45027024"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 45027024, container: ".js-paper-rank-work_45027024", }); });</script></li><li class="js-percentile-work_45027024 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 45027024; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_45027024"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_45027024 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="45027024"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 45027024; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=45027024]").text(description); $(".js-view-count-work_45027024").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_45027024").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="45027024"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=45027024]'), work: {"id":45027024,"title":"Multimedia Presentation of Musical Instruments","created_at":"2021-02-01T07:59:02.661-08:00","url":"https://www.academia.edu/45027024/Multimedia_Presentation_of_Musical_Instruments?f_ri=80799","dom_id":"work_45027024","summary":"The problem presented in the paper belongs to a wide subject concerning the use of multimedia technology for the improvement of educational activities in museums and for attracting the audience with objects of art. Several examples of temporal and regular multimedia performances in galleries are known in Poland and abroad, but still the technology is not fully used in traditional museums. In the paper, the case study of multimedia presentation devoted to the collection of the historical instruments from the Museum of Musical Instruments in Poznań is described. By their nature, musical instruments are interactive, but for the reasons of security and costs, only on rare occasions may visitors listen to their sound. Multimedia can change this situation. The inspiration for creating the multimedia presentation was the 250th Anniversary of Wolfgang Amadeus Mozart birth. The historical 18th century instruments from the collection of the museum accompanied by the music of the composer have been virtually exposed. Shown during the \"Museums Night\" in May 2006, the presentation has gained interest of hundreds of guests and proved useful for future educational actions.","downloadable_attachments":[{"id":65576391,"asset_id":45027024,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":184487419,"first_name":"Ewa","last_name":"Łukasik","domain_name":"wats-kompozyty","page_name":"EwaŁukasik","display_name":"Ewa Łukasik","profile_url":"https://wats-kompozyty.academia.edu/Ewa%C5%81ukasik?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_76327401" data-work_id="76327401" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/76327401/Vibration_transmission_through_plate_beam_structures_typical_of_lightweight_buildings_Applicability_and_limitations_of_fundamental_theories">Vibration transmission through plate/beam structures typical of lightweight buildings: Applicability and limitations of fundamental theories</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This paper examines the modelling of vibration transmission through plate/beam structures typical of lightweight buildings. Key experiments have been carried out on simple structures to identify the applicability and limitations of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_76327401" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This paper examines the modelling of vibration transmission through plate/beam structures typical of lightweight buildings. Key experiments have been carried out on simple structures to identify the applicability and limitations of fundamental theories. The systems tested included a single plate connected along its centre to a beam, two parallel plates attached along their centre to a beam (plates opposite or offset), and four plates connected along their edges to a beam. The analysis focused in particular on the applicability of modelling a beam as a one-dimensional element in point connected systems (widely spaced screws in terms of bending wavelength). Statistical energy analysis (SEA) was the framework of analysis used for all predictions, but the theories examined were independent from SEA. The results obtained indicate that simple point models are only applicable to the single plate and beam system, and to the parallel opposite plates connected along their centre to a beam; even then, the applicability of such models is limited to low and mid frequencies (below 2 kHz for the structures tested). Transmission between two parallel plates connected to a beam with screws closely spaced was also examined, and it was found that rigid and pinned line predictions can provide limits for transmission between panels on the same side of a wall (where junctions with shallow beams tend to behave rigidly, whilst junctions with deep beams are better modelled as pinned).</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/76327401" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="536f6b093babc9d423b78787103cb277" rel="nofollow" data-download="{"attachment_id":84069172,"asset_id":76327401,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/84069172/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="55014730" href="https://hw.academia.edu/LaurentGalbrun">Laurent Galbrun</a><script data-card-contents-for-user="55014730" type="text/json">{"id":55014730,"first_name":"Laurent","last_name":"Galbrun","domain_name":"hw","page_name":"LaurentGalbrun","display_name":"Laurent Galbrun","profile_url":"https://hw.academia.edu/LaurentGalbrun?f_ri=80799","photo":"https://0.academia-photos.com/55014730/14506196/15389027/s65_laurent.galbrun.gif"}</script></span></span></li><li class="js-paper-rank-work_76327401 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="76327401"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 76327401, container: ".js-paper-rank-work_76327401", }); 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$(".js-view-count[data-work-id=76327401]").text(description); $(".js-view-count-work_76327401").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_76327401").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="76327401"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">14</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="48" rel="nofollow" href="https://www.academia.edu/Documents/in/Engineering">Engineering</a>, <script data-card-contents-for-ri="48" type="text/json">{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="499" rel="nofollow" href="https://www.academia.edu/Documents/in/Acoustics">Acoustics</a>, <script data-card-contents-for-ri="499" type="text/json">{"id":499,"name":"Acoustics","url":"https://www.academia.edu/Documents/in/Acoustics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="1372" rel="nofollow" href="https://www.academia.edu/Documents/in/Architecture">Architecture</a><script data-card-contents-for-ri="1372" type="text/json">{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=76327401]'), work: {"id":76327401,"title":"Vibration transmission through plate/beam structures typical of lightweight buildings: Applicability and limitations of fundamental theories","created_at":"2022-04-13T06:30:37.194-07:00","url":"https://www.academia.edu/76327401/Vibration_transmission_through_plate_beam_structures_typical_of_lightweight_buildings_Applicability_and_limitations_of_fundamental_theories?f_ri=80799","dom_id":"work_76327401","summary":"This paper examines the modelling of vibration transmission through plate/beam structures typical of lightweight buildings. Key experiments have been carried out on simple structures to identify the applicability and limitations of fundamental theories. The systems tested included a single plate connected along its centre to a beam, two parallel plates attached along their centre to a beam (plates opposite or offset), and four plates connected along their edges to a beam. The analysis focused in particular on the applicability of modelling a beam as a one-dimensional element in point connected systems (widely spaced screws in terms of bending wavelength). Statistical energy analysis (SEA) was the framework of analysis used for all predictions, but the theories examined were independent from SEA. The results obtained indicate that simple point models are only applicable to the single plate and beam system, and to the parallel opposite plates connected along their centre to a beam; even then, the applicability of such models is limited to low and mid frequencies (below 2 kHz for the structures tested). Transmission between two parallel plates connected to a beam with screws closely spaced was also examined, and it was found that rigid and pinned line predictions can provide limits for transmission between panels on the same side of a wall (where junctions with shallow beams tend to behave rigidly, whilst junctions with deep beams are better modelled as pinned).","downloadable_attachments":[{"id":84069172,"asset_id":76327401,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":55014730,"first_name":"Laurent","last_name":"Galbrun","domain_name":"hw","page_name":"LaurentGalbrun","display_name":"Laurent Galbrun","profile_url":"https://hw.academia.edu/LaurentGalbrun?f_ri=80799","photo":"https://0.academia-photos.com/55014730/14506196/15389027/s65_laurent.galbrun.gif"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=80799","nofollow":true},{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":499,"name":"Acoustics","url":"https://www.academia.edu/Documents/in/Acoustics?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":5187,"name":"Statistical Analysis","url":"https://www.academia.edu/Documents/in/Statistical_Analysis?f_ri=80799"},{"id":6177,"name":"Modeling","url":"https://www.academia.edu/Documents/in/Modeling?f_ri=80799"},{"id":23077,"name":"Vibration","url":"https://www.academia.edu/Documents/in/Vibration?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":236747,"name":"Building Acoustics","url":"https://www.academia.edu/Documents/in/Building_Acoustics?f_ri=80799"},{"id":289482,"name":"Statistical Energy Analysis","url":"https://www.academia.edu/Documents/in/Statistical_Energy_Analysis?f_ri=80799"},{"id":753013,"name":"Properties of materials","url":"https://www.academia.edu/Documents/in/Properties_of_materials?f_ri=80799"},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799"},{"id":1890646,"name":"Structural Testing","url":"https://www.academia.edu/Documents/in/Structural_Testing?f_ri=80799"},{"id":1974375,"name":"Sound Transmission Loss","url":"https://www.academia.edu/Documents/in/Sound_Transmission_Loss?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_76051568" data-work_id="76051568" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/76051568/Fokker_Planck_description_of_the_scattering_of_radio_frequency_waves_at_the_plasma_edge">Fokker–Planck description of the scattering of radio frequency waves at the plasma edge</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In magnetic fusion devices, radio frequency ͑rf͒ waves in the electron cyclotron ͑EC͒ and lower hybrid ͑LH͒ range of frequencies are being commonly used to modify the plasma current profile. In ITER, EC waves are expected to stabilize the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_76051568" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In magnetic fusion devices, radio frequency ͑rf͒ waves in the electron cyclotron ͑EC͒ and lower hybrid ͑LH͒ range of frequencies are being commonly used to modify the plasma current profile. In ITER, EC waves are expected to stabilize the neoclassical tearing mode ͑NTM͒ by providing current in the island region ͓R. Aymar et al., Nucl. Fusion 41, 1301 ͑2001͔͒. The appearance of NTMs severely limits the plasma pressure and leads to the degradation of plasma confinement. LH waves could be used in ITER to modify the current profile closer to the edge of the plasma. These rf waves propagate from the excitation structures to the core of the plasma through an edge region, which is characterized by turbulence-in particular, density fluctuations. These fluctuations, in the form of blobs, can modify the propagation properties of the waves by refraction. In this paper, the effect on rf due to randomly distributed blobs in the edge region is studied. The waves are represented as geometric optics rays and the refractive scattering from a distribution of blobs is formulated as a Fokker-Planck equation. The scattering can have two diffusive effects-one in real space and the other in wave vector space. The scattering can modify the trajectory of rays into the plasma and it can affect the wave vector spectrum. The refraction of EC waves, for example, could make them miss the intended target region where the NTMs occur. The broadening of the wave vector spectrum could broaden the wave generated current profile. The Fokker-Planck formalism for diffusion in real space and wave vector space is used to study the effect of density blobs on EC and LH waves in an ITER type of plasma environment. For EC waves the refractive effects become important since the distance of propagation from the edge to the core in ITER is of the order of a meter. The diffusion in wave vector space is small. For LH waves the refractive effects are insignificant but the diffusion in wave vector space is important. The theoretical model is general enough to study the effect of density blobs on all propagating cold plasma waves.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/76051568" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="acded13952d5a96f50ef62d59e0cb6e8" rel="nofollow" data-download="{"attachment_id":83736708,"asset_id":76051568,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/83736708/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="35504920" href="https://independent.academia.edu/AbhayRam">Abhay Ram</a><script data-card-contents-for-user="35504920" type="text/json">{"id":35504920,"first_name":"Abhay","last_name":"Ram","domain_name":"independent","page_name":"AbhayRam","display_name":"Abhay Ram","profile_url":"https://independent.academia.edu/AbhayRam?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_76051568 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="76051568"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 76051568, container: ".js-paper-rank-work_76051568", }); });</script></li><li class="js-percentile-work_76051568 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76051568; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_76051568"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_76051568 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="76051568"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76051568; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76051568]").text(description); $(".js-view-count-work_76051568").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_76051568").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="76051568"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">11</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="64388" rel="nofollow" href="https://www.academia.edu/Documents/in/Electromagnetic_Waves">Electromagnetic Waves</a>, <script data-card-contents-for-ri="64388" type="text/json">{"id":64388,"name":"Electromagnetic Waves","url":"https://www.academia.edu/Documents/in/Electromagnetic_Waves?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="159012" rel="nofollow" href="https://www.academia.edu/Documents/in/Radio_Frequency">Radio Frequency</a>, <script data-card-contents-for-ri="159012" type="text/json">{"id":159012,"name":"Radio Frequency","url":"https://www.academia.edu/Documents/in/Radio_Frequency?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="163654" rel="nofollow" href="https://www.academia.edu/Documents/in/FOkker_Planck_Equation">FOkker Planck Equation</a><script data-card-contents-for-ri="163654" type="text/json">{"id":163654,"name":"FOkker Planck Equation","url":"https://www.academia.edu/Documents/in/FOkker_Planck_Equation?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=76051568]'), work: {"id":76051568,"title":"Fokker–Planck description of the scattering of radio frequency waves at the plasma edge","created_at":"2022-04-10T19:26:44.656-07:00","url":"https://www.academia.edu/76051568/Fokker_Planck_description_of_the_scattering_of_radio_frequency_waves_at_the_plasma_edge?f_ri=80799","dom_id":"work_76051568","summary":"In magnetic fusion devices, radio frequency ͑rf͒ waves in the electron cyclotron ͑EC͒ and lower hybrid ͑LH͒ range of frequencies are being commonly used to modify the plasma current profile. In ITER, EC waves are expected to stabilize the neoclassical tearing mode ͑NTM͒ by providing current in the island region ͓R. Aymar et al., Nucl. Fusion 41, 1301 ͑2001͔͒. The appearance of NTMs severely limits the plasma pressure and leads to the degradation of plasma confinement. LH waves could be used in ITER to modify the current profile closer to the edge of the plasma. These rf waves propagate from the excitation structures to the core of the plasma through an edge region, which is characterized by turbulence-in particular, density fluctuations. These fluctuations, in the form of blobs, can modify the propagation properties of the waves by refraction. In this paper, the effect on rf due to randomly distributed blobs in the edge region is studied. The waves are represented as geometric optics rays and the refractive scattering from a distribution of blobs is formulated as a Fokker-Planck equation. The scattering can have two diffusive effects-one in real space and the other in wave vector space. The scattering can modify the trajectory of rays into the plasma and it can affect the wave vector spectrum. The refraction of EC waves, for example, could make them miss the intended target region where the NTMs occur. The broadening of the wave vector spectrum could broaden the wave generated current profile. The Fokker-Planck formalism for diffusion in real space and wave vector space is used to study the effect of density blobs on EC and LH waves in an ITER type of plasma environment. For EC waves the refractive effects become important since the distance of propagation from the edge to the core in ITER is of the order of a meter. The diffusion in wave vector space is small. For LH waves the refractive effects are insignificant but the diffusion in wave vector space is important. The theoretical model is general enough to study the effect of density blobs on all propagating cold plasma waves.","downloadable_attachments":[{"id":83736708,"asset_id":76051568,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":35504920,"first_name":"Abhay","last_name":"Ram","domain_name":"independent","page_name":"AbhayRam","display_name":"Abhay Ram","profile_url":"https://independent.academia.edu/AbhayRam?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":64388,"name":"Electromagnetic Waves","url":"https://www.academia.edu/Documents/in/Electromagnetic_Waves?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":159012,"name":"Radio Frequency","url":"https://www.academia.edu/Documents/in/Radio_Frequency?f_ri=80799","nofollow":true},{"id":163654,"name":"FOkker Planck Equation","url":"https://www.academia.edu/Documents/in/FOkker_Planck_Equation?f_ri=80799","nofollow":true},{"id":260010,"name":"Wave propagation","url":"https://www.academia.edu/Documents/in/Wave_propagation?f_ri=80799"},{"id":321836,"name":"Spectrum","url":"https://www.academia.edu/Documents/in/Spectrum?f_ri=80799"},{"id":685326,"name":"Boundary Layer","url":"https://www.academia.edu/Documents/in/Boundary_Layer?f_ri=80799"},{"id":732001,"name":"Vector Space","url":"https://www.academia.edu/Documents/in/Vector_Space?f_ri=80799"},{"id":1154248,"name":"Theoretical Model","url":"https://www.academia.edu/Documents/in/Theoretical_Model?f_ri=80799"},{"id":1403220,"name":"Geometric Optics","url":"https://www.academia.edu/Documents/in/Geometric_Optics?f_ri=80799"},{"id":1671813,"name":"Boundary Effect","url":"https://www.academia.edu/Documents/in/Boundary_Effect?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_75919596" data-work_id="75919596" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/75919596/Radiation_of_Langmuir_solitons">Radiation of Langmuir solitons</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/75919596" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="2f695c513e82df91217baccd1b688aed" rel="nofollow" data-download="{"attachment_id":83587234,"asset_id":75919596,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/83587234/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="42267230" href="https://uni-bayreuth.academia.edu/HansSchamel">Hans Schamel</a><script data-card-contents-for-user="42267230" type="text/json">{"id":42267230,"first_name":"Hans","last_name":"Schamel","domain_name":"uni-bayreuth","page_name":"HansSchamel","display_name":"Hans Schamel","profile_url":"https://uni-bayreuth.academia.edu/HansSchamel?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_75919596 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="75919596"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 75919596, container: ".js-paper-rank-work_75919596", }); 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The temperature range examined was... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_71745777" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">New absolute measurements, by the transient hot-wire technique, of the thermal conductivity of n-hexadecane and binary mixtures of n-hexadecane with ethanol and n-decane with butanol are presented. The temperature range examined was 295-345 K and the pressure atmospheric. The concentrations of the mixtures studied were 92% (by weight) of n-hexadecane and 30 and 70% (by weight) of n-decane. The overall uncertainty in the reported thermal conductivity data is estimated to be _+0.5%, an estimate confirmed by the measurement of the thermal conductivity of water. A recently extended semiempirical scheme for the prediction of the thermal conductivity of mixtures from the pure components is used to correlate and predict the thermal conductivity of these mixtures, as a function of both composition and temperature.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/71745777" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="0403d335864bb991d1b9480276330fec" rel="nofollow" data-download="{"attachment_id":80961725,"asset_id":71745777,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/80961725/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="212267864" href="https://auth.academia.edu/MarcAssael">Marc J . 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The temperature range examined was 295-345 K and the pressure atmospheric. The concentrations of the mixtures studied were 92% (by weight) of n-hexadecane and 30 and 70% (by weight) of n-decane. The overall uncertainty in the reported thermal conductivity data is estimated to be _+0.5%, an estimate confirmed by the measurement of the thermal conductivity of water. A recently extended semiempirical scheme for the prediction of the thermal conductivity of mixtures from the pure components is used to correlate and predict the thermal conductivity of these mixtures, as a function of both composition and temperature.","downloadable_attachments":[{"id":80961725,"asset_id":71745777,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":212267864,"first_name":"Marc","last_name":"Assael","domain_name":"auth","page_name":"MarcAssael","display_name":"Marc J . Assael","profile_url":"https://auth.academia.edu/MarcAssael?f_ri=80799","photo":"https://0.academia-photos.com/212267864/71421942/59866008/s65_marc.assael.jpeg"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":246758,"name":"Thermal Conductivity","url":"https://www.academia.edu/Documents/in/Thermal_Conductivity?f_ri=80799","nofollow":true},{"id":846269,"name":"Thermophysics","url":"https://www.academia.edu/Documents/in/Thermophysics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_66594890 coauthored" data-work_id="66594890" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/66594890/Transport_property_measurements_on_the_IUPAC_sample_of_1_1_1_2_tetrafluoroethane_R134a_">Transport property measurements on the IUPAC sample of 1, 1, 1, 2-tetrafluoroethane (R134a)</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This paper reports the results of an international project coordinated by the Subcommittee on Transport Properties of Commission I.2 of the International Union of Pure and Applied Chemistry. The project has been conducted to investigate... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_66594890" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This paper reports the results of an international project coordinated by the Subcommittee on Transport Properties of Commission I.2 of the International Union of Pure and Applied Chemistry. The project has been conducted to investigate the large discrepancies between the results reported by various authors for the transport properties of R134a and culminates the effort which was initially described in 1995. The project has involved the remeasurement of the transport properties of a single sample of R134a in nine laboratories throughout the world in order to test the hypothesis that at least part of the discrepancy could be attributed to the purity of the samples. This paper provides an intercomparison of the new experimental results obtained for the viscosity 1</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/66594890" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="6cdca3d37a4def42bb2de1b864a7ab2e" rel="nofollow" data-download="{"attachment_id":77724206,"asset_id":66594890,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/77724206/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="60233540" href="https://independent.academia.edu/CarlosCastro348">Carlos A N D Castro</a><script data-card-contents-for-user="60233540" type="text/json">{"id":60233540,"first_name":"Carlos","last_name":"Castro","domain_name":"independent","page_name":"CarlosCastro348","display_name":"Carlos A N D Castro","profile_url":"https://independent.academia.edu/CarlosCastro348?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-66594890">+1</span><div class="hidden js-additional-users-66594890"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/RichardAPerkins">Richard A. 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The project has been conducted to investigate the large discrepancies between the results reported by various authors for the transport properties of R134a and culminates the effort which was initially described in 1995. The project has involved the remeasurement of the transport properties of a single sample of R134a in nine laboratories throughout the world in order to test the hypothesis that at least part of the discrepancy could be attributed to the purity of the samples. This paper provides an intercomparison of the new experimental results obtained for the viscosity 1","downloadable_attachments":[{"id":77724206,"asset_id":66594890,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":60233540,"first_name":"Carlos","last_name":"Castro","domain_name":"independent","page_name":"CarlosCastro348","display_name":"Carlos A N D Castro","profile_url":"https://independent.academia.edu/CarlosCastro348?f_ri=80799","photo":"/images/s65_no_pic.png"},{"id":214561382,"first_name":"Richard A.","last_name":"Perkins","domain_name":"independent","page_name":"RichardAPerkins","display_name":"Richard A. Perkins","profile_url":"https://independent.academia.edu/RichardAPerkins?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":4512,"name":"Light Scattering","url":"https://www.academia.edu/Documents/in/Light_Scattering?f_ri=80799","nofollow":true},{"id":60653,"name":"Transport Properties","url":"https://www.academia.edu/Documents/in/Transport_Properties?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":153240,"name":"Reference Data","url":"https://www.academia.edu/Documents/in/Reference_Data?f_ri=80799","nofollow":true},{"id":174781,"name":"Oscillations","url":"https://www.academia.edu/Documents/in/Oscillations?f_ri=80799"},{"id":234860,"name":"Steady state","url":"https://www.academia.edu/Documents/in/Steady_state?f_ri=80799"},{"id":246758,"name":"Thermal Conductivity","url":"https://www.academia.edu/Documents/in/Thermal_Conductivity?f_ri=80799"},{"id":846269,"name":"Thermophysics","url":"https://www.academia.edu/Documents/in/Thermophysics?f_ri=80799"},{"id":1290017,"name":"Round Robin","url":"https://www.academia.edu/Documents/in/Round_Robin?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_63404064" data-work_id="63404064" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/63404064/Time_Domain_Calculations_of_Sound_Interactions_With_Outdoor_Ground_Surfaces">Time-Domain Calculations of Sound Interactions With Outdoor Ground Surfaces</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A time-domain formulation for sound propagation in rigid-frame porous media, including waveform attenuation and dispersion, is developed. The new formulation is based on inversion of the relaxation functions from a previous model [Wilson... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_63404064" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A time-domain formulation for sound propagation in rigid-frame porous media, including waveform attenuation and dispersion, is developed. The new formulation is based on inversion of the relaxation functions from a previous model [Wilson DK, Ostashev VE, Collier SL. J Acoust Soc Am 2004;116:1889-92], thereby casting the convolution integrals in a form amenable to numerical implementation. Numerical techniques are developed that accurately implement the relaxational equations and transparently reduce to previous results in low-and high-frequency limits. The techniques are demonstrated on calculations of outdoor sound propagation involving hills, barriers, and ground surfaces with various material properties. We also compare the relaxation formulation to a widely applied phenomenological model developed by Zwikker and Kosten. The two models can be made equivalent if the resistance constant, structure constant, and compression modulus in the ZK model are allowed to be weakly frequency dependent. But if the ZK parameters are taken to be constant, as is typically the case, the relaxation model provides more accurate calculations of attenuation by acoustically soft porous materials such as snow, gravel, and forest litter.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/63404064" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="362361cb08c56e1a76a766d41e6e7112" rel="nofollow" data-download="{"attachment_id":75845779,"asset_id":63404064,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/75845779/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="87727723" href="https://independent.academia.edu/DavidMarlin1">David Marlin</a><script data-card-contents-for-user="87727723" type="text/json">{"id":87727723,"first_name":"David","last_name":"Marlin","domain_name":"independent","page_name":"DavidMarlin1","display_name":"David Marlin","profile_url":"https://independent.academia.edu/DavidMarlin1?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_63404064 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="63404064"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 63404064, container: ".js-paper-rank-work_63404064", }); 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The new formulation is based on inversion of the relaxation functions from a previous model [Wilson DK, Ostashev VE, Collier SL. J Acoust Soc Am 2004;116:1889-92], thereby casting the convolution integrals in a form amenable to numerical implementation. Numerical techniques are developed that accurately implement the relaxational equations and transparently reduce to previous results in low-and high-frequency limits. The techniques are demonstrated on calculations of outdoor sound propagation involving hills, barriers, and ground surfaces with various material properties. We also compare the relaxation formulation to a widely applied phenomenological model developed by Zwikker and Kosten. The two models can be made equivalent if the resistance constant, structure constant, and compression modulus in the ZK model are allowed to be weakly frequency dependent. But if the ZK parameters are taken to be constant, as is typically the case, the relaxation model provides more accurate calculations of attenuation by acoustically soft porous materials such as snow, gravel, and forest litter.","downloadable_attachments":[{"id":75845779,"asset_id":63404064,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":87727723,"first_name":"David","last_name":"Marlin","domain_name":"independent","page_name":"DavidMarlin1","display_name":"David Marlin","profile_url":"https://independent.academia.edu/DavidMarlin1?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":1372,"name":"Architecture","url":"https://www.academia.edu/Documents/in/Architecture?f_ri=80799","nofollow":true},{"id":2802,"name":"Turbulence","url":"https://www.academia.edu/Documents/in/Turbulence?f_ri=80799","nofollow":true},{"id":9032,"name":"Interaction","url":"https://www.academia.edu/Documents/in/Interaction?f_ri=80799","nofollow":true},{"id":23890,"name":"Comparative Study","url":"https://www.academia.edu/Documents/in/Comparative_Study?f_ri=80799"},{"id":29263,"name":"Aeroacoustics","url":"https://www.academia.edu/Documents/in/Aeroacoustics?f_ri=80799"},{"id":48458,"name":"High Frequency","url":"https://www.academia.edu/Documents/in/High_Frequency?f_ri=80799"},{"id":60658,"name":"Numerical Simulation","url":"https://www.academia.edu/Documents/in/Numerical_Simulation?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":90637,"name":"Porous Media","url":"https://www.academia.edu/Documents/in/Porous_Media?f_ri=80799"},{"id":176756,"name":"FORMULATION","url":"https://www.academia.edu/Documents/in/FORMULATION?f_ri=80799"},{"id":349439,"name":"Frequency Dependence","url":"https://www.academia.edu/Documents/in/Frequency_Dependence?f_ri=80799"},{"id":508740,"name":"Porous Material","url":"https://www.academia.edu/Documents/in/Porous_Material?f_ri=80799"},{"id":991005,"name":"Time Domain","url":"https://www.academia.edu/Documents/in/Time_Domain?f_ri=80799"},{"id":1001094,"name":"Material Properties","url":"https://www.academia.edu/Documents/in/Material_Properties?f_ri=80799"},{"id":1234852,"name":"Noise Barriers","url":"https://www.academia.edu/Documents/in/Noise_Barriers?f_ri=80799"},{"id":1280929,"name":"Applied Acoustics","url":"https://www.academia.edu/Documents/in/Applied_Acoustics?f_ri=80799"},{"id":1926798,"name":"PHENOMENOLOGICAL MODEL","url":"https://www.academia.edu/Documents/in/PHENOMENOLOGICAL_MODEL?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_47797990" data-work_id="47797990" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/47797990/_P_V_T_x_Measurements_of_the_system_benzene_1_3_5_trimethylbenzene_at_temperatures_from_298_15_to_328_15_K_and_at_pressures_up_to_40_MPa">(P, V, T, x) Measurements of the system benzene + 1,3,5-trimethylbenzene at temperatures from 298.15 to 328.15 K and at pressures up to 40 MPa</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Densities were measured for the liquid benzene and 1,3,5-trimethylbenzene, and for nine of their mixtures at four temperatures between 298.15 and 328.15 K and at pressures up to 40 MPa. An apparatus for density measurements of liquids and... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47797990" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Densities were measured for the liquid benzene and 1,3,5-trimethylbenzene, and for nine of their mixtures at four temperatures between 298.15 and 328.15 K and at pressures up to 40 MPa. An apparatus for density measurements of liquids and liquid mixtures whose main part is a high-pressure vibrating-tube densimeter working in a static mode was used for the measurement. The density data were fitted to the Tait equation and the isothermal compressibilities were calculated with the aid of this equation. Excess molar volumes were also calculated from the densities and fitted to the Redlich-Kister equation.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/47797990" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5d5614c4916b8f770bf734e92feea122" rel="nofollow" data-download="{"attachment_id":66735067,"asset_id":47797990,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/66735067/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="42117283" href="https://independent.academia.edu/ZdenekWagner">Zdenek Wagner</a><script data-card-contents-for-user="42117283" type="text/json">{"id":42117283,"first_name":"Zdenek","last_name":"Wagner","domain_name":"independent","page_name":"ZdenekWagner","display_name":"Zdenek Wagner","profile_url":"https://independent.academia.edu/ZdenekWagner?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_47797990 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="47797990"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 47797990, container: ".js-paper-rank-work_47797990", }); 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$(".js-view-count[data-work-id=47797990]").text(description); $(".js-view-count-work_47797990").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_47797990").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="47797990"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="4107" rel="nofollow" href="https://www.academia.edu/Documents/in/High_Pressure">High Pressure</a>, <script data-card-contents-for-ri="4107" type="text/json">{"id":4107,"name":"High Pressure","url":"https://www.academia.edu/Documents/in/High_Pressure?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="629119" rel="nofollow" href="https://www.academia.edu/Documents/in/Fluid_phase_equilibria">Fluid phase equilibria</a><script data-card-contents-for-ri="629119" type="text/json">{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=47797990]'), work: {"id":47797990,"title":"(P, V, T, x) Measurements of the system benzene + 1,3,5-trimethylbenzene at temperatures from 298.15 to 328.15 K and at pressures up to 40 MPa","created_at":"2021-04-30T16:22:46.630-07:00","url":"https://www.academia.edu/47797990/_P_V_T_x_Measurements_of_the_system_benzene_1_3_5_trimethylbenzene_at_temperatures_from_298_15_to_328_15_K_and_at_pressures_up_to_40_MPa?f_ri=80799","dom_id":"work_47797990","summary":"Densities were measured for the liquid benzene and 1,3,5-trimethylbenzene, and for nine of their mixtures at four temperatures between 298.15 and 328.15 K and at pressures up to 40 MPa. An apparatus for density measurements of liquids and liquid mixtures whose main part is a high-pressure vibrating-tube densimeter working in a static mode was used for the measurement. The density data were fitted to the Tait equation and the isothermal compressibilities were calculated with the aid of this equation. Excess molar volumes were also calculated from the densities and fitted to the Redlich-Kister equation.","downloadable_attachments":[{"id":66735067,"asset_id":47797990,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":42117283,"first_name":"Zdenek","last_name":"Wagner","domain_name":"independent","page_name":"ZdenekWagner","display_name":"Zdenek Wagner","profile_url":"https://independent.academia.edu/ZdenekWagner?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":4107,"name":"High Pressure","url":"https://www.academia.edu/Documents/in/High_Pressure?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_71307091" data-work_id="71307091" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" rel="nofollow" href="https://www.academia.edu/71307091/Influence_of_the_Electric_Guitars_Fingerboard_Wood_on_Guitarists_Perception">Influence of the Electric Guitar's Fingerboard Wood on Guitarists' Perception</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">ABSTRACT The sound of a solid body electric guitar comes from the loudspeaker transducing into sound the string velocity. Because of mechanical string-structure coupling, the string vibration, and therefore the sound, substantially... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_71307091" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">ABSTRACT The sound of a solid body electric guitar comes from the loudspeaker transducing into sound the string velocity. Because of mechanical string-structure coupling, the string vibration, and therefore the sound, substantially depends on the lutherie parameters. This study focuses on the comparison between ebony-fingerboard and rosewood-fingerboard guitars: is a change in the fingerboard wood perceived by the guitar players? In order to test the hypothesis that it is actually perceived, a psychological investigation is carried out. Two experimental methods are used: a free sorting task with recorded stimuli from the guitars (listening test) and a free verbalisation task where the guitarists play the guitars. In the listening test, the guitarists perceive differences between guitars, but the resulting clusters do not show an ebony/rosewood dichotomy. A linguistic analysis of the verbalisations exhibits psychological descriptors that are relevant for the discrimination of the wood of the fingerboard: PRECISION (referring to how each note stands out from others), and to a lesser extent ATTACK (referring to the guitar&amp;#39;s response to musician&amp;#39;s gesture) and BALANCE (referring to the frequency content). This study is part of a broader project aiming at establishing an explicite relation between mechanics, perception, and lutherie. A physical interpretation of the psychologically-relevant descriptors is eventually proposed in order to use them as hypotheses in a further hypothetico-deductive approach starting from physics and using psychophysical methods.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/71307091" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="51063629" href="https://independent.academia.edu/danieledubois">daniele dubois</a><script data-card-contents-for-user="51063629" type="text/json">{"id":51063629,"first_name":"daniele","last_name":"dubois","domain_name":"independent","page_name":"danieledubois","display_name":"daniele dubois","profile_url":"https://independent.academia.edu/danieledubois?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_71307091 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="71307091"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 71307091, container: ".js-paper-rank-work_71307091", }); 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Because of mechanical string-structure coupling, the string vibration, and therefore the sound, substantially depends on the lutherie parameters. This study focuses on the comparison between ebony-fingerboard and rosewood-fingerboard guitars: is a change in the fingerboard wood perceived by the guitar players? In order to test the hypothesis that it is actually perceived, a psychological investigation is carried out. Two experimental methods are used: a free sorting task with recorded stimuli from the guitars (listening test) and a free verbalisation task where the guitarists play the guitars. In the listening test, the guitarists perceive differences between guitars, but the resulting clusters do not show an ebony/rosewood dichotomy. A linguistic analysis of the verbalisations exhibits psychological descriptors that are relevant for the discrimination of the wood of the fingerboard: PRECISION (referring to how each note stands out from others), and to a lesser extent ATTACK (referring to the guitar\u0026amp;#39;s response to musician\u0026amp;#39;s gesture) and BALANCE (referring to the frequency content). This study is part of a broader project aiming at establishing an explicite relation between mechanics, perception, and lutherie. A physical interpretation of the psychologically-relevant descriptors is eventually proposed in order to use them as hypotheses in a further hypothetico-deductive approach starting from physics and using psychophysical methods.","downloadable_attachments":[],"ordered_authors":[{"id":51063629,"first_name":"daniele","last_name":"dubois","domain_name":"independent","page_name":"danieledubois","display_name":"daniele dubois","profile_url":"https://independent.academia.edu/danieledubois?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":867,"name":"Perception","url":"https://www.academia.edu/Documents/in/Perception?f_ri=80799","nofollow":true},{"id":8088,"name":"Sound","url":"https://www.academia.edu/Documents/in/Sound?f_ri=80799","nofollow":true},{"id":8967,"name":"Musical acoustics","url":"https://www.academia.edu/Documents/in/Musical_acoustics?f_ri=80799","nofollow":true},{"id":15674,"name":"Linguistics","url":"https://www.academia.edu/Documents/in/Linguistics?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":135707,"name":"Electric Guitar","url":"https://www.academia.edu/Documents/in/Electric_Guitar?f_ri=80799"},{"id":140024,"name":"Wood science and technology","url":"https://www.academia.edu/Documents/in/Wood_science_and_technology?f_ri=80799"},{"id":642232,"name":"Verbalization","url":"https://www.academia.edu/Documents/in/Verbalization?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_66807452" data-work_id="66807452" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/66807452/FRW_cosmology_in_f_Q_T_gravity">FRW cosmology in f(Q,T) gravity</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In this paper, we considered the study of Friedmann–Robertson–Walker (FRW) model in the framework of [Formula: see text] gravity, an extension of symmetric teleparallel gravity, recently defined by Xu et al. [[Formula: see text] gravity,... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_66807452" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In this paper, we considered the study of Friedmann–Robertson–Walker (FRW) model in the framework of [Formula: see text] gravity, an extension of symmetric teleparallel gravity, recently defined by Xu et al. [[Formula: see text] gravity, Eur. Phys. J. C 79 (2019) 708]. The nonlinear model [Formula: see text], where [Formula: see text] and [Formula: see text] are constants, is taken into account. The equation of state of perfect fluid is assumed and 31 points of Hubble data are used to constrain the value of model parameter. To explore the evolution of the universe, the numerical solutions of cosmological implications, such as Hubble parameter, deceleration parameter, apparent magnitude and luminosity distance, are determined and the energy conditions are examined. The theoretical results of Hubble parameter are compared with [Formula: see text]CDM model. Further, 57 Supernova data (42 from Supernova cosmology project and 15 from Calán/Tolono supernova survey) are also used to have c...</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/66807452" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="54be2f7a0d3b580d42ce2ed1da01f94d" rel="nofollow" data-download="{"attachment_id":77857867,"asset_id":66807452,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/77857867/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="78534713" href="https://independent.academia.edu/NishaGodani">Nisha Godani</a><script data-card-contents-for-user="78534713" type="text/json">{"id":78534713,"first_name":"Nisha","last_name":"Godani","domain_name":"independent","page_name":"NishaGodani","display_name":"Nisha Godani","profile_url":"https://independent.academia.edu/NishaGodani?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_66807452 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="66807452"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 66807452, container: ".js-paper-rank-work_66807452", }); 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[[Formula: see text] gravity, Eur. Phys. J. C 79 (2019) 708]. The nonlinear model [Formula: see text], where [Formula: see text] and [Formula: see text] are constants, is taken into account. The equation of state of perfect fluid is assumed and 31 points of Hubble data are used to constrain the value of model parameter. To explore the evolution of the universe, the numerical solutions of cosmological implications, such as Hubble parameter, deceleration parameter, apparent magnitude and luminosity distance, are determined and the energy conditions are examined. The theoretical results of Hubble parameter are compared with [Formula: see text]CDM model. Further, 57 Supernova data (42 from Supernova cosmology project and 15 from Calán/Tolono supernova survey) are also used to have c...","downloadable_attachments":[{"id":77857867,"asset_id":66807452,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":78534713,"first_name":"Nisha","last_name":"Godani","domain_name":"independent","page_name":"NishaGodani","display_name":"Nisha Godani","profile_url":"https://independent.academia.edu/NishaGodani?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_61401590" data-work_id="61401590" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/61401590/STRAIGHT_exploitation_of_the_other_aspect_of_VOCODER_Perceptually_isomorphic_decomposition_of_speech_sounds">STRAIGHT, exploitation of the other aspect of VOCODER: Perceptually isomorphic decomposition of speech sounds</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">STRAIGHT, a speech analysis, modification synthesis system, is an extension of the classical channel VOCODER that exploits the advantages of progress in information processing technologies and a new conceptualization of the role of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_61401590" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">STRAIGHT, a speech analysis, modification synthesis system, is an extension of the classical channel VOCODER that exploits the advantages of progress in information processing technologies and a new conceptualization of the role of repetitive structures in speech sounds. This review outlines historical backgrounds, architecture, underlying principles, and representative applications of STRAIGHT.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/61401590" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="2492d8aa2939fc3540293c0cca738dd4" rel="nofollow" data-download="{"attachment_id":74442737,"asset_id":61401590,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/74442737/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="37838820" href="https://wakayama-u.academia.edu/HidekiKawahara">Hideki Kawahara</a><script data-card-contents-for-user="37838820" type="text/json">{"id":37838820,"first_name":"Hideki","last_name":"Kawahara","domain_name":"wakayama-u","page_name":"HidekiKawahara","display_name":"Hideki Kawahara","profile_url":"https://wakayama-u.academia.edu/HidekiKawahara?f_ri=80799","photo":"https://0.academia-photos.com/37838820/10627831/11863443/s65_hideki.kawahara.jpg"}</script></span></span></li><li class="js-paper-rank-work_61401590 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="61401590"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 61401590, container: ".js-paper-rank-work_61401590", }); 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$(".js-view-count[data-work-id=61401590]").text(description); $(".js-view-count-work_61401590").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_61401590").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="61401590"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">9</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="60" rel="nofollow" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="2342" rel="nofollow" href="https://www.academia.edu/Documents/in/Speech_Synthesis">Speech Synthesis</a>, <script data-card-contents-for-ri="2342" type="text/json">{"id":2342,"name":"Speech Synthesis","url":"https://www.academia.edu/Documents/in/Speech_Synthesis?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="5391" rel="nofollow" href="https://www.academia.edu/Documents/in/Speech_perception">Speech perception</a>, <script data-card-contents-for-ri="5391" type="text/json">{"id":5391,"name":"Speech perception","url":"https://www.academia.edu/Documents/in/Speech_perception?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="11984" rel="nofollow" href="https://www.academia.edu/Documents/in/Speech_Recognition">Speech Recognition</a><script data-card-contents-for-ri="11984" type="text/json">{"id":11984,"name":"Speech Recognition","url":"https://www.academia.edu/Documents/in/Speech_Recognition?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=61401590]'), work: {"id":61401590,"title":"STRAIGHT, exploitation of the other aspect of VOCODER: Perceptually isomorphic decomposition of speech sounds","created_at":"2021-11-09T06:25:20.472-08:00","url":"https://www.academia.edu/61401590/STRAIGHT_exploitation_of_the_other_aspect_of_VOCODER_Perceptually_isomorphic_decomposition_of_speech_sounds?f_ri=80799","dom_id":"work_61401590","summary":"STRAIGHT, a speech analysis, modification synthesis system, is an extension of the classical channel VOCODER that exploits the advantages of progress in information processing technologies and a new conceptualization of the role of repetitive structures in speech sounds. This review outlines historical backgrounds, architecture, underlying principles, and representative applications of STRAIGHT.","downloadable_attachments":[{"id":74442737,"asset_id":61401590,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":37838820,"first_name":"Hideki","last_name":"Kawahara","domain_name":"wakayama-u","page_name":"HidekiKawahara","display_name":"Hideki Kawahara","profile_url":"https://wakayama-u.academia.edu/HidekiKawahara?f_ri=80799","photo":"https://0.academia-photos.com/37838820/10627831/11863443/s65_hideki.kawahara.jpg"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=80799","nofollow":true},{"id":2342,"name":"Speech Synthesis","url":"https://www.academia.edu/Documents/in/Speech_Synthesis?f_ri=80799","nofollow":true},{"id":5391,"name":"Speech perception","url":"https://www.academia.edu/Documents/in/Speech_perception?f_ri=80799","nofollow":true},{"id":11984,"name":"Speech Recognition","url":"https://www.academia.edu/Documents/in/Speech_Recognition?f_ri=80799","nofollow":true},{"id":36837,"name":"Information Processing","url":"https://www.academia.edu/Documents/in/Information_Processing?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":95360,"name":"Spectral analysis","url":"https://www.academia.edu/Documents/in/Spectral_analysis?f_ri=80799"},{"id":368258,"name":"Speech analysis","url":"https://www.academia.edu/Documents/in/Speech_analysis?f_ri=80799"},{"id":1986543,"name":"PACS numbers","url":"https://www.academia.edu/Documents/in/PACS_numbers?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_60135632" data-work_id="60135632" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/60135632/Plasma_oscillations_in_Hall_thrusters">Plasma oscillations in Hall thrusters</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The nature of oscillations in the 1 kHz-60 MHz frequency range that have been observed during operation of Hall thrusters is quantitatively discussed. Contours of various plasma parameters measured inside the accelerating channel of a... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_60135632" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The nature of oscillations in the 1 kHz-60 MHz frequency range that have been observed during operation of Hall thrusters is quantitatively discussed. Contours of various plasma parameters measured inside the accelerating channel of a typical Hall thruster are used to evaluate the various stability criteria and dispersion relations of oscillations that are suspected to occur. A band by band up-to-date overview of the oscillations is carried out with a description of their observed behavior and a discussion of their nature and dependencies through comparison of the calculated contours to reported observations. The discussion encompasses the excitation of low frequency azimuthal drift waves that can form a rotating spoke, axially propagating ''transit-time'' oscillations, azimuthal drift waves, ionization instability-type waves, and wave emission peculiar to weakly ionized inhomogeneous plasmas in crossed electric and magnetic fields.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/60135632" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="cdc2787b31ab3848414288ec3871723d" rel="nofollow" data-download="{"attachment_id":73709836,"asset_id":60135632,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/73709836/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="69064670" href="https://independent.academia.edu/EdgarChoueiri1">Edgar Choueiri</a><script data-card-contents-for-user="69064670" type="text/json">{"id":69064670,"first_name":"Edgar","last_name":"Choueiri","domain_name":"independent","page_name":"EdgarChoueiri1","display_name":"Edgar Choueiri","profile_url":"https://independent.academia.edu/EdgarChoueiri1?f_ri=80799","photo":"https://0.academia-photos.com/69064670/42670201/34162330/s65_edgar.choueiri.jpg"}</script></span></span></li><li class="js-paper-rank-work_60135632 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="60135632"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 60135632, container: ".js-paper-rank-work_60135632", }); 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$(".js-view-count[data-work-id=60135632]").text(description); $(".js-view-count-work_60135632").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_60135632").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="60135632"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="721" rel="nofollow" href="https://www.academia.edu/Documents/in/Magnetohydrodynamics">Magnetohydrodynamics</a>, <script data-card-contents-for-ri="721" type="text/json">{"id":721,"name":"Magnetohydrodynamics","url":"https://www.academia.edu/Documents/in/Magnetohydrodynamics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="30372" rel="nofollow" href="https://www.academia.edu/Documents/in/Low_Frequency">Low Frequency</a>, <script data-card-contents-for-ri="30372" type="text/json">{"id":30372,"name":"Low Frequency","url":"https://www.academia.edu/Documents/in/Low_Frequency?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="151145" rel="nofollow" href="https://www.academia.edu/Documents/in/Dispersion_Relation">Dispersion Relation</a><script data-card-contents-for-ri="151145" type="text/json">{"id":151145,"name":"Dispersion Relation","url":"https://www.academia.edu/Documents/in/Dispersion_Relation?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=60135632]'), work: {"id":60135632,"title":"Plasma oscillations in Hall thrusters","created_at":"2021-10-27T04:40:23.094-07:00","url":"https://www.academia.edu/60135632/Plasma_oscillations_in_Hall_thrusters?f_ri=80799","dom_id":"work_60135632","summary":"The nature of oscillations in the 1 kHz-60 MHz frequency range that have been observed during operation of Hall thrusters is quantitatively discussed. Contours of various plasma parameters measured inside the accelerating channel of a typical Hall thruster are used to evaluate the various stability criteria and dispersion relations of oscillations that are suspected to occur. A band by band up-to-date overview of the oscillations is carried out with a description of their observed behavior and a discussion of their nature and dependencies through comparison of the calculated contours to reported observations. The discussion encompasses the excitation of low frequency azimuthal drift waves that can form a rotating spoke, axially propagating ''transit-time'' oscillations, azimuthal drift waves, ionization instability-type waves, and wave emission peculiar to weakly ionized inhomogeneous plasmas in crossed electric and magnetic fields.","downloadable_attachments":[{"id":73709836,"asset_id":60135632,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":69064670,"first_name":"Edgar","last_name":"Choueiri","domain_name":"independent","page_name":"EdgarChoueiri1","display_name":"Edgar Choueiri","profile_url":"https://independent.academia.edu/EdgarChoueiri1?f_ri=80799","photo":"https://0.academia-photos.com/69064670/42670201/34162330/s65_edgar.choueiri.jpg"}],"research_interests":[{"id":721,"name":"Magnetohydrodynamics","url":"https://www.academia.edu/Documents/in/Magnetohydrodynamics?f_ri=80799","nofollow":true},{"id":30372,"name":"Low Frequency","url":"https://www.academia.edu/Documents/in/Low_Frequency?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":151145,"name":"Dispersion Relation","url":"https://www.academia.edu/Documents/in/Dispersion_Relation?f_ri=80799","nofollow":true},{"id":174781,"name":"Oscillations","url":"https://www.academia.edu/Documents/in/Oscillations?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_55156393" data-work_id="55156393" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/55156393/Mobile_agents_affect_worm_spreading_in_wireless_ad_hoc_networks">Mobile agents affect worm spreading in wireless ad hoc networks</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Considering the dynamic nature of portable computing devices with wireless communication capability, an extended model is introduced for worm spreading in the wireless ad hoc network, with a population of mobile agents in a planar... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_55156393" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Considering the dynamic nature of portable computing devices with wireless communication capability, an extended model is introduced for worm spreading in the wireless ad hoc network, with a population of mobile agents in a planar distribution, starting from an initial infected seed. The effect of agents' mobility on worm spreading is investigated via extensive Monte Carlo simulations. The threshold behavior and the dynamics of worm epidemics in the wireless networks are greatly affected by both agents' mobility and spatial and temporal correlations. The medium access control mechanism for the wireless communication promotes the sensitivity of the spreading dynamics to agents' mobility.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/55156393" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="23c54bb58c489f03246f39cc8426e521" rel="nofollow" data-download="{"attachment_id":71162729,"asset_id":55156393,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/71162729/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="32185066" href="https://independent.academia.edu/ZiGangHuang">Zi-Gang Huang</a><script data-card-contents-for-user="32185066" type="text/json">{"id":32185066,"first_name":"Zi-Gang","last_name":"Huang","domain_name":"independent","page_name":"ZiGangHuang","display_name":"Zi-Gang Huang","profile_url":"https://independent.academia.edu/ZiGangHuang?f_ri=80799","photo":"https://0.academia-photos.com/32185066/9616710/10711858/s65_zi-gang.huang.jpg"}</script></span></span></li><li class="js-paper-rank-work_55156393 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="55156393"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 55156393, container: ".js-paper-rank-work_55156393", }); 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$(".js-view-count[data-work-id=55156393]").text(description); $(".js-view-count-work_55156393").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_55156393").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="55156393"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">11</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="318" rel="nofollow" href="https://www.academia.edu/Documents/in/Mathematical_Physics">Mathematical Physics</a>, <script data-card-contents-for-ri="318" type="text/json">{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="859" rel="nofollow" href="https://www.academia.edu/Documents/in/Communication">Communication</a>, <script data-card-contents-for-ri="859" type="text/json">{"id":859,"name":"Communication","url":"https://www.academia.edu/Documents/in/Communication?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="4392" rel="nofollow" href="https://www.academia.edu/Documents/in/Monte_Carlo_Simulation">Monte Carlo Simulation</a>, <script data-card-contents-for-ri="4392" type="text/json">{"id":4392,"name":"Monte Carlo Simulation","url":"https://www.academia.edu/Documents/in/Monte_Carlo_Simulation?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="54856" rel="nofollow" href="https://www.academia.edu/Documents/in/Network_Dynamics">Network Dynamics</a><script data-card-contents-for-ri="54856" type="text/json">{"id":54856,"name":"Network Dynamics","url":"https://www.academia.edu/Documents/in/Network_Dynamics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=55156393]'), work: {"id":55156393,"title":"Mobile agents affect worm spreading in wireless ad hoc networks","created_at":"2021-10-03T08:48:27.563-07:00","url":"https://www.academia.edu/55156393/Mobile_agents_affect_worm_spreading_in_wireless_ad_hoc_networks?f_ri=80799","dom_id":"work_55156393","summary":"Considering the dynamic nature of portable computing devices with wireless communication capability, an extended model is introduced for worm spreading in the wireless ad hoc network, with a population of mobile agents in a planar distribution, starting from an initial infected seed. The effect of agents' mobility on worm spreading is investigated via extensive Monte Carlo simulations. The threshold behavior and the dynamics of worm epidemics in the wireless networks are greatly affected by both agents' mobility and spatial and temporal correlations. The medium access control mechanism for the wireless communication promotes the sensitivity of the spreading dynamics to agents' mobility.","downloadable_attachments":[{"id":71162729,"asset_id":55156393,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":32185066,"first_name":"Zi-Gang","last_name":"Huang","domain_name":"independent","page_name":"ZiGangHuang","display_name":"Zi-Gang Huang","profile_url":"https://independent.academia.edu/ZiGangHuang?f_ri=80799","photo":"https://0.academia-photos.com/32185066/9616710/10711858/s65_zi-gang.huang.jpg"}],"research_interests":[{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true},{"id":859,"name":"Communication","url":"https://www.academia.edu/Documents/in/Communication?f_ri=80799","nofollow":true},{"id":4392,"name":"Monte Carlo Simulation","url":"https://www.academia.edu/Documents/in/Monte_Carlo_Simulation?f_ri=80799","nofollow":true},{"id":54856,"name":"Network Dynamics","url":"https://www.academia.edu/Documents/in/Network_Dynamics?f_ri=80799","nofollow":true},{"id":65429,"name":"Wireless Network","url":"https://www.academia.edu/Documents/in/Wireless_Network?f_ri=80799"},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":149428,"name":"Temporal Correlation","url":"https://www.academia.edu/Documents/in/Temporal_Correlation?f_ri=80799"},{"id":423253,"name":"Mobile Agent","url":"https://www.academia.edu/Documents/in/Mobile_Agent?f_ri=80799"},{"id":516036,"name":"Medium Access Control","url":"https://www.academia.edu/Documents/in/Medium_Access_Control?f_ri=80799"},{"id":1232975,"name":"Wireless Communication","url":"https://www.academia.edu/Documents/in/Wireless_Communication-1?f_ri=80799"},{"id":1276229,"name":"Wireless Ad Hoc Network","url":"https://www.academia.edu/Documents/in/Wireless_Ad_Hoc_Network?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_52776322" data-work_id="52776322" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/52776322/How_not_to_teach_Lorentz_covariance_of_the_Dirac_equation">How (not) to teach Lorentz covariance of the Dirac equation</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In the textbook proofs of Lorentz covariance of the Dirac equation, one treats the wave function as a spinor and gamma matrices as scalars, leading to a quite complicated formalism with several pedagogic drawbacks. As an alternative, I... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_52776322" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In the textbook proofs of Lorentz covariance of the Dirac equation, one treats the wave function as a spinor and gamma matrices as scalars, leading to a quite complicated formalism with several pedagogic drawbacks. As an alternative, I propose to teach Dirac equation and its Lorentz covariance by using a much simpler, but physically equivalent formalism, in which these drawbacks do not appear. In this alternative formalism, the wave function transforms as a scalar and gamma matrices as components of a vector, such that the standard physically relevant bilinear combinations do not change their transformation properties. The alternative formalism allows also a natural construction of some additional non-standard bilinear combinations with well-defined transformation properties.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/52776322" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="f6a43b1b87cb7b3a39bac1a27f80a197" rel="nofollow" data-download="{"attachment_id":69878538,"asset_id":52776322,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/69878538/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="61184551" href="https://independent.academia.edu/NikolicHrvoje">Hrvoje Nikolic</a><script data-card-contents-for-user="61184551" type="text/json">{"id":61184551,"first_name":"Hrvoje","last_name":"Nikolic","domain_name":"independent","page_name":"NikolicHrvoje","display_name":"Hrvoje Nikolic","profile_url":"https://independent.academia.edu/NikolicHrvoje?f_ri=80799","photo":"https://0.academia-photos.com/61184551/23284247/22371310/s65_hrvoje.nikolic.jpg"}</script></span></span></li><li class="js-paper-rank-work_52776322 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="52776322"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 52776322, container: ".js-paper-rank-work_52776322", }); 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$(".js-view-count[data-work-id=52776322]").text(description); $(".js-view-count-work_52776322").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_52776322").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="52776322"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="143488" rel="nofollow" href="https://www.academia.edu/Documents/in/Dirac_equation">Dirac equation</a>, <script data-card-contents-for-ri="143488" type="text/json">{"id":143488,"name":"Dirac equation","url":"https://www.academia.edu/Documents/in/Dirac_equation?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="431989" rel="nofollow" href="https://www.academia.edu/Documents/in/Wave_Function">Wave Function</a><script data-card-contents-for-ri="431989" type="text/json">{"id":431989,"name":"Wave Function","url":"https://www.academia.edu/Documents/in/Wave_Function?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=52776322]'), work: {"id":52776322,"title":"How (not) to teach Lorentz covariance of the Dirac equation","created_at":"2021-09-18T22:45:28.916-07:00","url":"https://www.academia.edu/52776322/How_not_to_teach_Lorentz_covariance_of_the_Dirac_equation?f_ri=80799","dom_id":"work_52776322","summary":"In the textbook proofs of Lorentz covariance of the Dirac equation, one treats the wave function as a spinor and gamma matrices as scalars, leading to a quite complicated formalism with several pedagogic drawbacks. As an alternative, I propose to teach Dirac equation and its Lorentz covariance by using a much simpler, but physically equivalent formalism, in which these drawbacks do not appear. In this alternative formalism, the wave function transforms as a scalar and gamma matrices as components of a vector, such that the standard physically relevant bilinear combinations do not change their transformation properties. The alternative formalism allows also a natural construction of some additional non-standard bilinear combinations with well-defined transformation properties.","downloadable_attachments":[{"id":69878538,"asset_id":52776322,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":61184551,"first_name":"Hrvoje","last_name":"Nikolic","domain_name":"independent","page_name":"NikolicHrvoje","display_name":"Hrvoje Nikolic","profile_url":"https://independent.academia.edu/NikolicHrvoje?f_ri=80799","photo":"https://0.academia-photos.com/61184551/23284247/22371310/s65_hrvoje.nikolic.jpg"}],"research_interests":[{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":143488,"name":"Dirac equation","url":"https://www.academia.edu/Documents/in/Dirac_equation?f_ri=80799","nofollow":true},{"id":431989,"name":"Wave Function","url":"https://www.academia.edu/Documents/in/Wave_Function?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_47897740 coauthored" data-work_id="47897740" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/47897740/New_activity_pattern_in_human_interactive_dynamics">New activity pattern in human interactive dynamics</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">We investigate the response function of human agents as demonstrated by written correspondence, uncovering a new universal pattern for how the reactive dynamics of individuals is distributed across the set of each agent's contacts. In... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47897740" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">We investigate the response function of human agents as demonstrated by written correspondence, uncovering a new universal pattern for how the reactive dynamics of individuals is distributed across the set of each agent's contacts. In long-term empirical data on email, we find that the set of response times considered separately for the messages to each different correspondent of a given writer, generate a family of heavy-tailed distributions, which have largely the same features for all agents, and whose characteristic times grow exponentially with the rank of each correspondent. We furthermore show that this universal behavioral pattern emerges robustly by considering weighted moving averages of the priorityconditioned response-time probabilities generated by a basic prioritization model. Our findings clarify how the range of priorities in the inputs from one's environment underpin and shape the dynamics of agents embedded in a net of reactive relations. These newly revealed activity patterns might be present in other general interactive environments, and constrain future models of communication and interaction networks, affecting their architecture and evolution.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/47897740" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5beb5d3e4542878ecd236eb26353d137" rel="nofollow" data-download="{"attachment_id":66788451,"asset_id":47897740,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/66788451/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="14666669" href="https://independent.academia.edu/AlbertoLovison">Alberto Lovison</a><script data-card-contents-for-user="14666669" type="text/json">{"id":14666669,"first_name":"Alberto","last_name":"Lovison","domain_name":"independent","page_name":"AlbertoLovison","display_name":"Alberto Lovison","profile_url":"https://independent.academia.edu/AlbertoLovison?f_ri=80799","photo":"https://0.academia-photos.com/14666669/3990052/4660974/s65_alberto.lovison.jpg_oh_be60aed6d4509174a262621d9850119a_oe_54421a0e___gda___1414161895_769528a3b0cd34e82621fee539f17217"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-47897740">+1</span><div class="hidden js-additional-users-47897740"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/GZanzotto">Giovanni Zanzotto</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-47897740'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-47897740').html(); } } new HoverPopover(popoverSettings); })();</script></li><li class="js-paper-rank-work_47897740 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="47897740"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 47897740, container: ".js-paper-rank-work_47897740", }); });</script></li><li class="js-percentile-work_47897740 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 47897740; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_47897740"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_47897740 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="47897740"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 47897740; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=47897740]").text(description); $(".js-view-count-work_47897740").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_47897740").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="47897740"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="318" rel="nofollow" href="https://www.academia.edu/Documents/in/Mathematical_Physics">Mathematical Physics</a>, <script data-card-contents-for-ri="318" type="text/json">{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a><script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=47897740]'), work: {"id":47897740,"title":"New activity pattern in human interactive dynamics","created_at":"2021-05-03T01:25:53.543-07:00","url":"https://www.academia.edu/47897740/New_activity_pattern_in_human_interactive_dynamics?f_ri=80799","dom_id":"work_47897740","summary":"We investigate the response function of human agents as demonstrated by written correspondence, uncovering a new universal pattern for how the reactive dynamics of individuals is distributed across the set of each agent's contacts. In long-term empirical data on email, we find that the set of response times considered separately for the messages to each different correspondent of a given writer, generate a family of heavy-tailed distributions, which have largely the same features for all agents, and whose characteristic times grow exponentially with the rank of each correspondent. We furthermore show that this universal behavioral pattern emerges robustly by considering weighted moving averages of the priorityconditioned response-time probabilities generated by a basic prioritization model. Our findings clarify how the range of priorities in the inputs from one's environment underpin and shape the dynamics of agents embedded in a net of reactive relations. These newly revealed activity patterns might be present in other general interactive environments, and constrain future models of communication and interaction networks, affecting their architecture and evolution.","downloadable_attachments":[{"id":66788451,"asset_id":47897740,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":14666669,"first_name":"Alberto","last_name":"Lovison","domain_name":"independent","page_name":"AlbertoLovison","display_name":"Alberto Lovison","profile_url":"https://independent.academia.edu/AlbertoLovison?f_ri=80799","photo":"https://0.academia-photos.com/14666669/3990052/4660974/s65_alberto.lovison.jpg_oh_be60aed6d4509174a262621d9850119a_oe_54421a0e___gda___1414161895_769528a3b0cd34e82621fee539f17217"},{"id":214826570,"first_name":"Giovanni","last_name":"Zanzotto","domain_name":"independent","page_name":"GZanzotto","display_name":"Giovanni Zanzotto","profile_url":"https://independent.academia.edu/GZanzotto?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_47543906" data-work_id="47543906" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/47543906/Transverse_heat_transfer_coefficient_in_the_dual_channel_ITER_TF_CICCs">Transverse heat transfer coefficient in the dual channel ITER TF CICCs</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Two ITER TF dual channel Cable-in-Conduit Conductors (CICCs) have been tested in the SULTAN test facility. The samples were heated either by foil heaters mounted on the outside of the conductor jacket or by induced AC losses. The... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47543906" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Two ITER TF dual channel Cable-in-Conduit Conductors (CICCs) have been tested in the SULTAN test facility. The samples were heated either by foil heaters mounted on the outside of the conductor jacket or by induced AC losses. The steady-state temperature response of several thermometers installed on the jacket surface as well as inside the cable were analyzed using the two-channel analytical model proposed by Renard et al. to obtain the equivalent transverse heat transfer coefficient between the bundle and central channel as a function of the mass flow rate. In addition, on the basis of the measured pressure drop and helium flow velocities, the friction factors for helium flow in the bundle and in the central channel were determined. The obtained results may serve as a reference for these cables.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/47543906" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="f54f6508ea939f3af95cbc60bb104707" rel="nofollow" data-download="{"attachment_id":66582095,"asset_id":47543906,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/66582095/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="41945484" href="https://zut.academia.edu/MonikaLewandowska">Monika Lewandowska</a><script data-card-contents-for-user="41945484" type="text/json">{"id":41945484,"first_name":"Monika","last_name":"Lewandowska","domain_name":"zut","page_name":"MonikaLewandowska","display_name":"Monika Lewandowska","profile_url":"https://zut.academia.edu/MonikaLewandowska?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_47543906 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="47543906"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 47543906, container: ".js-paper-rank-work_47543906", }); });</script></li><li class="js-percentile-work_47543906 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 47543906; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_47543906"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_47543906 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="47543906"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 47543906; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=47543906]").text(description); $(".js-view-count-work_47543906").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_47543906").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="47543906"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">11</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="506" rel="nofollow" href="https://www.academia.edu/Documents/in/Cryogenics">Cryogenics</a>, <script data-card-contents-for-ri="506" type="text/json">{"id":506,"name":"Cryogenics","url":"https://www.academia.edu/Documents/in/Cryogenics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="44039" rel="nofollow" href="https://www.academia.edu/Documents/in/AC_Loss">AC Loss</a>, <script data-card-contents-for-ri="44039" type="text/json">{"id":44039,"name":"AC Loss","url":"https://www.academia.edu/Documents/in/AC_Loss?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="186189" rel="nofollow" href="https://www.academia.edu/Documents/in/Heat_transfer_coefficient">Heat transfer coefficient</a><script data-card-contents-for-ri="186189" type="text/json">{"id":186189,"name":"Heat transfer coefficient","url":"https://www.academia.edu/Documents/in/Heat_transfer_coefficient?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=47543906]'), work: {"id":47543906,"title":"Transverse heat transfer coefficient in the dual channel ITER TF CICCs","created_at":"2021-04-23T00:41:56.464-07:00","url":"https://www.academia.edu/47543906/Transverse_heat_transfer_coefficient_in_the_dual_channel_ITER_TF_CICCs?f_ri=80799","dom_id":"work_47543906","summary":"Two ITER TF dual channel Cable-in-Conduit Conductors (CICCs) have been tested in the SULTAN test facility. The samples were heated either by foil heaters mounted on the outside of the conductor jacket or by induced AC losses. The steady-state temperature response of several thermometers installed on the jacket surface as well as inside the cable were analyzed using the two-channel analytical model proposed by Renard et al. to obtain the equivalent transverse heat transfer coefficient between the bundle and central channel as a function of the mass flow rate. In addition, on the basis of the measured pressure drop and helium flow velocities, the friction factors for helium flow in the bundle and in the central channel were determined. The obtained results may serve as a reference for these cables.","downloadable_attachments":[{"id":66582095,"asset_id":47543906,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":41945484,"first_name":"Monika","last_name":"Lewandowska","domain_name":"zut","page_name":"MonikaLewandowska","display_name":"Monika Lewandowska","profile_url":"https://zut.academia.edu/MonikaLewandowska?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":506,"name":"Cryogenics","url":"https://www.academia.edu/Documents/in/Cryogenics?f_ri=80799","nofollow":true},{"id":44039,"name":"AC Loss","url":"https://www.academia.edu/Documents/in/AC_Loss?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":186189,"name":"Heat transfer coefficient","url":"https://www.academia.edu/Documents/in/Heat_transfer_coefficient?f_ri=80799","nofollow":true},{"id":234860,"name":"Steady state","url":"https://www.academia.edu/Documents/in/Steady_state?f_ri=80799"},{"id":331203,"name":"Pressure Drop","url":"https://www.academia.edu/Documents/in/Pressure_Drop?f_ri=80799"},{"id":413300,"name":"Analytical Model","url":"https://www.academia.edu/Documents/in/Analytical_Model?f_ri=80799"},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering?f_ri=80799"},{"id":601516,"name":"Flow Velocity","url":"https://www.academia.edu/Documents/in/Flow_Velocity?f_ri=80799"},{"id":898062,"name":"Flow Rate","url":"https://www.academia.edu/Documents/in/Flow_Rate?f_ri=80799"},{"id":2003310,"name":"Friction Factor","url":"https://www.academia.edu/Documents/in/Friction_Factor?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_36024104" data-work_id="36024104" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/36024104/Correlation_and_prediction_of_solute_transfer_to_chloroalkanes_from_both_water_and_the_gas_phase">Correlation and prediction of solute transfer to chloroalkanes from both water and the gas phase</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Data have been compiled from the published literature on the partition coefficients of solutes and vapors into chloroform, carbon tetrachloride, dichloromethane and 1-chlorobutane from both water and from the gas phase. The logarithms of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_36024104" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Data have been compiled from the published literature on the partition coefficients of solutes and vapors into chloroform, carbon tetrachloride, dichloromethane and 1-chlorobutane from both water and from the gas phase. The logarithms of the water-to-chloroalkane (log P) and gas-tochloroalkane partition coefficients (log K) are correlated with the Abraham solvation parameter model. The derived correlations describe the observed log P and log K values within standard deviations of about 0.13 to 0.20 log units. For chloroform and carbon tetrachloride, the derived correlations were validated using training set and test set analyses. 2</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/36024104" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="d113e72ac5fa033092e0cf6b3970da31" rel="nofollow" data-download="{"attachment_id":55910927,"asset_id":36024104,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/55910927/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="33030476" href="https://ucl.academia.edu/MichaelAbraham">Michael Abraham</a><script data-card-contents-for-user="33030476" type="text/json">{"id":33030476,"first_name":"Michael","last_name":"Abraham","domain_name":"ucl","page_name":"MichaelAbraham","display_name":"Michael Abraham","profile_url":"https://ucl.academia.edu/MichaelAbraham?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_36024104 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="36024104"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 36024104, container: ".js-paper-rank-work_36024104", }); 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$(".js-view-count[data-work-id=36024104]").text(description); $(".js-view-count-work_36024104").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_36024104").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="36024104"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">9</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="2215" rel="nofollow" href="https://www.academia.edu/Documents/in/Water">Water</a>, <script data-card-contents-for-ri="2215" type="text/json">{"id":2215,"name":"Water","url":"https://www.academia.edu/Documents/in/Water?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="7968" rel="nofollow" href="https://www.academia.edu/Documents/in/Prediction">Prediction</a>, <script data-card-contents-for-ri="7968" type="text/json">{"id":7968,"name":"Prediction","url":"https://www.academia.edu/Documents/in/Prediction?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="69841" rel="nofollow" href="https://www.academia.edu/Documents/in/Standard_Deviation">Standard Deviation</a><script data-card-contents-for-ri="69841" type="text/json">{"id":69841,"name":"Standard Deviation","url":"https://www.academia.edu/Documents/in/Standard_Deviation?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=36024104]'), work: {"id":36024104,"title":"Correlation and prediction of solute transfer to chloroalkanes from both water and the gas phase","created_at":"2018-02-26T16:21:38.814-08:00","url":"https://www.academia.edu/36024104/Correlation_and_prediction_of_solute_transfer_to_chloroalkanes_from_both_water_and_the_gas_phase?f_ri=80799","dom_id":"work_36024104","summary":"Data have been compiled from the published literature on the partition coefficients of solutes and vapors into chloroform, carbon tetrachloride, dichloromethane and 1-chlorobutane from both water and from the gas phase. The logarithms of the water-to-chloroalkane (log P) and gas-tochloroalkane partition coefficients (log K) are correlated with the Abraham solvation parameter model. The derived correlations describe the observed log P and log K values within standard deviations of about 0.13 to 0.20 log units. For chloroform and carbon tetrachloride, the derived correlations were validated using training set and test set analyses. 2","downloadable_attachments":[{"id":55910927,"asset_id":36024104,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":33030476,"first_name":"Michael","last_name":"Abraham","domain_name":"ucl","page_name":"MichaelAbraham","display_name":"Michael Abraham","profile_url":"https://ucl.academia.edu/MichaelAbraham?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":2215,"name":"Water","url":"https://www.academia.edu/Documents/in/Water?f_ri=80799","nofollow":true},{"id":7968,"name":"Prediction","url":"https://www.academia.edu/Documents/in/Prediction?f_ri=80799","nofollow":true},{"id":69841,"name":"Standard Deviation","url":"https://www.academia.edu/Documents/in/Standard_Deviation?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":81504,"name":"Correlation","url":"https://www.academia.edu/Documents/in/Correlation?f_ri=80799"},{"id":205581,"name":"Partition Coefficient","url":"https://www.academia.edu/Documents/in/Partition_Coefficient?f_ri=80799"},{"id":390063,"name":"Carbon Tetrachloride","url":"https://www.academia.edu/Documents/in/Carbon_Tetrachloride?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_33891242" data-work_id="33891242" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/33891242/Calculation_of_the_interfacial_tension_of_the_methane_water_system_with_the_linear_gradient_theory">Calculation of the interfacial tension of the methane–water system with the linear gradient theory</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The linear gradient theory (LGT) combined with the Soave-Redlich-Kwong (SRK EoS) and the Peng-Robinson (PR EoS) equations of state has been used to correlate the interfacial tension data of the methane-water system. The pure component... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_33891242" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The linear gradient theory (LGT) combined with the Soave-Redlich-Kwong (SRK EoS) and the Peng-Robinson (PR EoS) equations of state has been used to correlate the interfacial tension data of the methane-water system. The pure component influence parameters and the binary interaction coefficient for the mixture influence parameter have been obtained for this system. The model was successfully applied to correlate the interfacial tension data set to within 2.3% for the linear gradient theory and the SRK EoS (LGT-SRK) and 2.5% for the linear gradient theory and PE EoS (LGT-PR). A posteriori comparison of data not used in the parameterisation were to within 3.2% for the LGT-SRK model and 2.7% for the LGT-PR model. An exhaustive literature review resulted in a large database for the investigation which covers a wide range of temperature and pressures. The results support the success of the linear gradient theory modelling approach for this system.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/33891242" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="98e1fe10d951a252d1a6334c0905f856" rel="nofollow" data-download="{"attachment_id":53865221,"asset_id":33891242,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/53865221/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="66455750" href="https://uib.academia.edu/Bj%C3%B8rnKvamme">Bjørn Kvamme</a><script data-card-contents-for-user="66455750" type="text/json">{"id":66455750,"first_name":"Bjørn","last_name":"Kvamme","domain_name":"uib","page_name":"BjørnKvamme","display_name":"Bjørn Kvamme","profile_url":"https://uib.academia.edu/Bj%C3%B8rnKvamme?f_ri=80799","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_33891242 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="33891242"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 33891242, container: ".js-paper-rank-work_33891242", }); 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$(".js-view-count[data-work-id=33891242]").text(description); $(".js-view-count-work_33891242").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_33891242").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="33891242"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">9</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="72" rel="nofollow" href="https://www.academia.edu/Documents/in/Chemical_Engineering">Chemical Engineering</a>, <script data-card-contents-for-ri="72" type="text/json">{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="2215" rel="nofollow" href="https://www.academia.edu/Documents/in/Water">Water</a>, <script data-card-contents-for-ri="2215" type="text/json">{"id":2215,"name":"Water","url":"https://www.academia.edu/Documents/in/Water?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="9355" rel="nofollow" href="https://www.academia.edu/Documents/in/Equations_of_State">Equations of State</a>, <script data-card-contents-for-ri="9355" type="text/json">{"id":9355,"name":"Equations of State","url":"https://www.academia.edu/Documents/in/Equations_of_State?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="44293" rel="nofollow" href="https://www.academia.edu/Documents/in/Literature_Review">Literature Review</a><script data-card-contents-for-ri="44293" type="text/json">{"id":44293,"name":"Literature Review","url":"https://www.academia.edu/Documents/in/Literature_Review?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=33891242]'), work: {"id":33891242,"title":"Calculation of the interfacial tension of the methane–water system with the linear gradient theory","created_at":"2017-07-15T06:55:29.892-07:00","url":"https://www.academia.edu/33891242/Calculation_of_the_interfacial_tension_of_the_methane_water_system_with_the_linear_gradient_theory?f_ri=80799","dom_id":"work_33891242","summary":"The linear gradient theory (LGT) combined with the Soave-Redlich-Kwong (SRK EoS) and the Peng-Robinson (PR EoS) equations of state has been used to correlate the interfacial tension data of the methane-water system. The pure component influence parameters and the binary interaction coefficient for the mixture influence parameter have been obtained for this system. The model was successfully applied to correlate the interfacial tension data set to within 2.3% for the linear gradient theory and the SRK EoS (LGT-SRK) and 2.5% for the linear gradient theory and PE EoS (LGT-PR). A posteriori comparison of data not used in the parameterisation were to within 3.2% for the LGT-SRK model and 2.7% for the LGT-PR model. An exhaustive literature review resulted in a large database for the investigation which covers a wide range of temperature and pressures. The results support the success of the linear gradient theory modelling approach for this system.","downloadable_attachments":[{"id":53865221,"asset_id":33891242,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":66455750,"first_name":"Bjørn","last_name":"Kvamme","domain_name":"uib","page_name":"BjørnKvamme","display_name":"Bjørn Kvamme","profile_url":"https://uib.academia.edu/Bj%C3%B8rnKvamme?f_ri=80799","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering?f_ri=80799","nofollow":true},{"id":2215,"name":"Water","url":"https://www.academia.edu/Documents/in/Water?f_ri=80799","nofollow":true},{"id":9355,"name":"Equations of State","url":"https://www.academia.edu/Documents/in/Equations_of_State?f_ri=80799","nofollow":true},{"id":44293,"name":"Literature Review","url":"https://www.academia.edu/Documents/in/Literature_Review?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799"},{"id":156347,"name":"Methane","url":"https://www.academia.edu/Documents/in/Methane?f_ri=80799"},{"id":165199,"name":"Interfacial Tension","url":"https://www.academia.edu/Documents/in/Interfacial_Tension?f_ri=80799"},{"id":629119,"name":"Fluid phase equilibria","url":"https://www.academia.edu/Documents/in/Fluid_phase_equilibria?f_ri=80799"},{"id":1320599,"name":"Equation of State","url":"https://www.academia.edu/Documents/in/Equation_of_State?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_1943979" data-work_id="1943979" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/1943979/Wall_boundary_conditions_for_high_order_finite_difference_schemes_in_computational_aeroacoustics">Wall boundary conditions for high-order finite-difference schemes in computational aeroacoustics</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">High-order finite-difference schemes are less dispersive and dissipative but, at the same time, more isotropic than low-order schemes. They are well suited for solving computational acoustics problems. High-order finite-difference... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_1943979" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">High-order finite-difference schemes are less dispersive and dissipative but, at the same time, more isotropic than low-order schemes. They are well suited for solving computational acoustics problems. High-order finite-difference equations, however, support extraneous wave solutions which bear no resemblance to the exact solution of the original partial differential equations. These extraneous wave solutions, which invariably degrade the quality of the numerical solutions, are usually generated when solid-wall boundary conditions are imposed. A set of numerical boundary conditions simulating the presence of a solid wall for high-order finitedifference schemes using a minimum number of ghost values is proposed. The effectiveness of the numerical boundary conditions in producing quality solutions is analyzed and demonstrated by comparing the results of direct numerical simulations and exact solutions.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/1943979" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="98fd6904db0a310145c683612d0a1291" rel="nofollow" data-download="{"attachment_id":50810674,"asset_id":1943979,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/50810674/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="2520615" href="https://independent.academia.edu/PrasanthKutchu">Prasanth Kutchu</a><script data-card-contents-for-user="2520615" type="text/json">{"id":2520615,"first_name":"Prasanth","last_name":"Kutchu","domain_name":"independent","page_name":"PrasanthKutchu","display_name":"Prasanth Kutchu","profile_url":"https://independent.academia.edu/PrasanthKutchu?f_ri=80799","photo":"https://0.academia-photos.com/2520615/785762/976481/s65_prasanth.kutchu.jpg"}</script></span></span></li><li class="js-paper-rank-work_1943979 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="1943979"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 1943979, container: ".js-paper-rank-work_1943979", }); });</script></li><li class="js-percentile-work_1943979 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1943979; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_1943979"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_1943979 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="1943979"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1943979; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1943979]").text(description); $(".js-view-count-work_1943979").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_1943979").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="1943979"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">9</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="305" rel="nofollow" href="https://www.academia.edu/Documents/in/Applied_Mathematics">Applied Mathematics</a>, <script data-card-contents-for-ri="305" type="text/json">{"id":305,"name":"Applied Mathematics","url":"https://www.academia.edu/Documents/in/Applied_Mathematics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="10719" rel="nofollow" href="https://www.academia.edu/Documents/in/Direct_Numerical_Simulation">Direct Numerical Simulation</a>, <script data-card-contents-for-ri="10719" type="text/json">{"id":10719,"name":"Direct Numerical Simulation","url":"https://www.academia.edu/Documents/in/Direct_Numerical_Simulation?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="194130" rel="nofollow" href="https://www.academia.edu/Documents/in/PARTIAL_DIFFERENTIAL_EQUATION">PARTIAL DIFFERENTIAL EQUATION</a><script data-card-contents-for-ri="194130" type="text/json">{"id":194130,"name":"PARTIAL DIFFERENTIAL EQUATION","url":"https://www.academia.edu/Documents/in/PARTIAL_DIFFERENTIAL_EQUATION?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=1943979]'), work: {"id":1943979,"title":"Wall boundary conditions for high-order finite-difference schemes in computational aeroacoustics","created_at":"2012-09-17T13:52:10.817-07:00","url":"https://www.academia.edu/1943979/Wall_boundary_conditions_for_high_order_finite_difference_schemes_in_computational_aeroacoustics?f_ri=80799","dom_id":"work_1943979","summary":"High-order finite-difference schemes are less dispersive and dissipative but, at the same time, more isotropic than low-order schemes. They are well suited for solving computational acoustics problems. High-order finite-difference equations, however, support extraneous wave solutions which bear no resemblance to the exact solution of the original partial differential equations. These extraneous wave solutions, which invariably degrade the quality of the numerical solutions, are usually generated when solid-wall boundary conditions are imposed. A set of numerical boundary conditions simulating the presence of a solid wall for high-order finitedifference schemes using a minimum number of ghost values is proposed. The effectiveness of the numerical boundary conditions in producing quality solutions is analyzed and demonstrated by comparing the results of direct numerical simulations and exact solutions.","downloadable_attachments":[{"id":50810674,"asset_id":1943979,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":2520615,"first_name":"Prasanth","last_name":"Kutchu","domain_name":"independent","page_name":"PrasanthKutchu","display_name":"Prasanth Kutchu","profile_url":"https://independent.academia.edu/PrasanthKutchu?f_ri=80799","photo":"https://0.academia-photos.com/2520615/785762/976481/s65_prasanth.kutchu.jpg"}],"research_interests":[{"id":305,"name":"Applied Mathematics","url":"https://www.academia.edu/Documents/in/Applied_Mathematics?f_ri=80799","nofollow":true},{"id":10719,"name":"Direct Numerical Simulation","url":"https://www.academia.edu/Documents/in/Direct_Numerical_Simulation?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":194130,"name":"PARTIAL DIFFERENTIAL EQUATION","url":"https://www.academia.edu/Documents/in/PARTIAL_DIFFERENTIAL_EQUATION?f_ri=80799","nofollow":true},{"id":452692,"name":"Finite Difference","url":"https://www.academia.edu/Documents/in/Finite_Difference?f_ri=80799"},{"id":867022,"name":"Boundary Condition","url":"https://www.academia.edu/Documents/in/Boundary_Condition?f_ri=80799"},{"id":896204,"name":"Numerical Solution","url":"https://www.academia.edu/Documents/in/Numerical_Solution?f_ri=80799"},{"id":1868639,"name":"Exact solution methods","url":"https://www.academia.edu/Documents/in/Exact_solution_methods?f_ri=80799"},{"id":2354906,"name":"Finite Difference Scheme","url":"https://www.academia.edu/Documents/in/Finite_Difference_Scheme?f_ri=80799"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_6161869" data-work_id="6161869" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/6161869/Photoacoustic_Analysis_of_Pigments_from_Archeological_Ceramics">Photoacoustic Analysis of Pigments from Archeological Ceramics</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Photoacoustic spectroscopy (PAS) is widely used for diverse applications in different areas. These include studies in material, environmental, and life sciences. In the present work the study of pigments from pottery surfaces and volumes... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_6161869" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Photoacoustic spectroscopy (PAS) is widely used for diverse applications in different areas. These include studies in material, environmental, and life sciences. In the present work the study of pigments from pottery surfaces and volumes of Mexican (Aztec) and Poblana cultures that were developed in central Mexico from 1325 to 1521 and 1521 to 1800, respectively, is reported. The optical absorption spectra from each archeological sample was obtained using PAS. The superficial spectra were also compared with standard color pigments and archeological registers. Complementary energy dispersive spectroscopy (EDS) analysis of these archeological potteries gave us their elemental composition which agreed with other studies about their composition and technology of the pottery manufacturing.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/6161869" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="171d7a27210956a23daad4f9366293b2" rel="nofollow" data-download="{"attachment_id":48990668,"asset_id":6161869,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/48990668/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="9370851" href="https://independent.academia.edu/AlfredoCruz1">Alfredo Cruz</a><script data-card-contents-for-user="9370851" type="text/json">{"id":9370851,"first_name":"Alfredo","last_name":"Cruz","domain_name":"independent","page_name":"AlfredoCruz1","display_name":"Alfredo Cruz","profile_url":"https://independent.academia.edu/AlfredoCruz1?f_ri=80799","photo":"https://0.academia-photos.com/9370851/72156878/60616003/s65_alfredo.cruz.jpeg"}</script></span></span></li><li class="js-paper-rank-work_6161869 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="6161869"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 6161869, container: ".js-paper-rank-work_6161869", }); 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$(".js-view-count[data-work-id=6161869]").text(description); $(".js-view-count-work_6161869").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_6161869").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="6161869"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="8014" rel="nofollow" href="https://www.academia.edu/Documents/in/Life_Sciences">Life Sciences</a>, <script data-card-contents-for-ri="8014" type="text/json">{"id":8014,"name":"Life Sciences","url":"https://www.academia.edu/Documents/in/Life_Sciences?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="846269" rel="nofollow" href="https://www.academia.edu/Documents/in/Thermophysics">Thermophysics</a>, <script data-card-contents-for-ri="846269" type="text/json">{"id":846269,"name":"Thermophysics","url":"https://www.academia.edu/Documents/in/Thermophysics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="907289" rel="nofollow" href="https://www.academia.edu/Documents/in/Energy_Dispersive_Spectroscopy">Energy Dispersive Spectroscopy</a><script data-card-contents-for-ri="907289" type="text/json">{"id":907289,"name":"Energy Dispersive Spectroscopy","url":"https://www.academia.edu/Documents/in/Energy_Dispersive_Spectroscopy?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=6161869]'), work: {"id":6161869,"title":"Photoacoustic Analysis of Pigments from Archeological Ceramics","created_at":"2014-02-21T10:27:48.789-08:00","url":"https://www.academia.edu/6161869/Photoacoustic_Analysis_of_Pigments_from_Archeological_Ceramics?f_ri=80799","dom_id":"work_6161869","summary":"Photoacoustic spectroscopy (PAS) is widely used for diverse applications in different areas. These include studies in material, environmental, and life sciences. In the present work the study of pigments from pottery surfaces and volumes of Mexican (Aztec) and Poblana cultures that were developed in central Mexico from 1325 to 1521 and 1521 to 1800, respectively, is reported. The optical absorption spectra from each archeological sample was obtained using PAS. The superficial spectra were also compared with standard color pigments and archeological registers. Complementary energy dispersive spectroscopy (EDS) analysis of these archeological potteries gave us their elemental composition which agreed with other studies about their composition and technology of the pottery manufacturing.","downloadable_attachments":[{"id":48990668,"asset_id":6161869,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":9370851,"first_name":"Alfredo","last_name":"Cruz","domain_name":"independent","page_name":"AlfredoCruz1","display_name":"Alfredo Cruz","profile_url":"https://independent.academia.edu/AlfredoCruz1?f_ri=80799","photo":"https://0.academia-photos.com/9370851/72156878/60616003/s65_alfredo.cruz.jpeg"}],"research_interests":[{"id":8014,"name":"Life Sciences","url":"https://www.academia.edu/Documents/in/Life_Sciences?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":846269,"name":"Thermophysics","url":"https://www.academia.edu/Documents/in/Thermophysics?f_ri=80799","nofollow":true},{"id":907289,"name":"Energy Dispersive Spectroscopy","url":"https://www.academia.edu/Documents/in/Energy_Dispersive_Spectroscopy?f_ri=80799","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_6480987" data-work_id="6480987" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/6480987/Modified_Zakharov_equations_for_plasmas_with_a_quantum_correction">Modified Zakharov equations for plasmas with a quantum correction</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Quantum Zakharov equations are obtained to describe the nonlinear interaction between quantum Langmuir waves and quantum ion-acoustic waves. These quantum Zakharov equations are applied to two model cases, namely the four-wave interaction... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_6480987" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Quantum Zakharov equations are obtained to describe the nonlinear interaction between quantum Langmuir waves and quantum ion-acoustic waves. These quantum Zakharov equations are applied to two model cases, namely the four-wave interaction and the decay instability. In the case of the four-wave instability, sufficiently large quantum effects tend to suppress the instability.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/6480987" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="c0c6dffad7f4eed1c572d7c5ede8b47d" rel="nofollow" data-download="{"attachment_id":48849346,"asset_id":6480987,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/48849346/download_file?st=MTc0MDIyMzU1NCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="10298039" href="https://independent.academia.edu/LuizPauloLunadeOliveira">Luiz Paulo Luna de Oliveira</a><script data-card-contents-for-user="10298039" type="text/json">{"id":10298039,"first_name":"Luiz Paulo","last_name":"Luna de Oliveira","domain_name":"independent","page_name":"LuizPauloLunadeOliveira","display_name":"Luiz Paulo Luna de Oliveira","profile_url":"https://independent.academia.edu/LuizPauloLunadeOliveira?f_ri=80799","photo":"https://0.academia-photos.com/10298039/3296130/3878796/s65_luiz_paulo.luna_de_oliveira.jpg"}</script></span></span></li><li class="js-paper-rank-work_6480987 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="6480987"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 6480987, container: ".js-paper-rank-work_6480987", }); 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$(".js-view-count[data-work-id=6480987]").text(description); $(".js-view-count-work_6480987").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_6480987").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="6480987"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">7</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="56340" rel="nofollow" href="https://www.academia.edu/Documents/in/Integer_quantum_hall_effect">Integer quantum hall effect</a>, <script data-card-contents-for-ri="56340" type="text/json">{"id":56340,"name":"Integer quantum hall effect","url":"https://www.academia.edu/Documents/in/Integer_quantum_hall_effect?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="80799" rel="nofollow" href="https://www.academia.edu/Documents/in/Classical_Physics">Classical Physics</a>, <script data-card-contents-for-ri="80799" type="text/json">{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="151145" rel="nofollow" href="https://www.academia.edu/Documents/in/Dispersion_Relation">Dispersion Relation</a>, <script data-card-contents-for-ri="151145" type="text/json">{"id":151145,"name":"Dispersion Relation","url":"https://www.academia.edu/Documents/in/Dispersion_Relation?f_ri=80799","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="174781" rel="nofollow" href="https://www.academia.edu/Documents/in/Oscillations">Oscillations</a><script data-card-contents-for-ri="174781" type="text/json">{"id":174781,"name":"Oscillations","url":"https://www.academia.edu/Documents/in/Oscillations?f_ri=80799","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=6480987]'), work: {"id":6480987,"title":"Modified Zakharov equations for plasmas with a quantum correction","created_at":"2014-03-20T00:41:43.595-07:00","url":"https://www.academia.edu/6480987/Modified_Zakharov_equations_for_plasmas_with_a_quantum_correction?f_ri=80799","dom_id":"work_6480987","summary":"Quantum Zakharov equations are obtained to describe the nonlinear interaction between quantum Langmuir waves and quantum ion-acoustic waves. These quantum Zakharov equations are applied to two model cases, namely the four-wave interaction and the decay instability. In the case of the four-wave instability, sufficiently large quantum effects tend to suppress the instability.","downloadable_attachments":[{"id":48849346,"asset_id":6480987,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":10298039,"first_name":"Luiz Paulo","last_name":"Luna de Oliveira","domain_name":"independent","page_name":"LuizPauloLunadeOliveira","display_name":"Luiz Paulo Luna de Oliveira","profile_url":"https://independent.academia.edu/LuizPauloLunadeOliveira?f_ri=80799","photo":"https://0.academia-photos.com/10298039/3296130/3878796/s65_luiz_paulo.luna_de_oliveira.jpg"}],"research_interests":[{"id":56340,"name":"Integer quantum hall effect","url":"https://www.academia.edu/Documents/in/Integer_quantum_hall_effect?f_ri=80799","nofollow":true},{"id":80799,"name":"Classical Physics","url":"https://www.academia.edu/Documents/in/Classical_Physics?f_ri=80799","nofollow":true},{"id":151145,"name":"Dispersion 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