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data-trace="false" data-dom-id="ProfileCheckPaperUpdate-react-component-97944781-69ef-41f9-a060-3c981087a95b"></div> <div id="ProfileCheckPaperUpdate-react-component-97944781-69ef-41f9-a060-3c981087a95b"></div> <div class="DesignSystem"><div class="onsite-ping" id="onsite-ping"></div></div><div class="profile-user-info DesignSystem"><div class="social-profile-container"><div class="left-panel-container"><div class="user-info-component-wrapper"><div class="user-summary-cta-container"><div class="user-summary-container"><div class="social-profile-avatar-container"><img class="profile-avatar u-positionAbsolute" border="0" alt="" src="//a.academia-assets.com/images/s200_no_pic.png" /></div><div class="title-container"><h1 class="ds2-5-heading-sans-serif-sm">Teng Zhou</h1><div class="affiliations-container fake-truncate js-profile-affiliations"><div><a class="u-tcGrayDarker" href="https://pledco.academia.edu/">Hainan University</a>, <a class="u-tcGrayDarker" 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class="user-stats-container"><a><div class="stat-container js-profile-followers"><p class="label">Followers</p><p class="data">5</p></div></a><a><div class="stat-container js-profile-followees" data-broccoli-component="user-info.followees-count" data-click-track="profile-expand-user-info-following"><p class="label">Following</p><p class="data">10</p></div></a><a><div class="stat-container js-profile-coauthors" data-broccoli-component="user-info.coauthors-count" data-click-track="profile-expand-user-info-coauthors"><p class="label">Co-authors</p><p class="data">3</p></div></a><span><div class="stat-container"><p class="label"><span class="js-profile-total-view-text">Public Views</span></p><p class="data"><span class="js-profile-view-count"></span></p></div></span></div><div class="user-bio-container"><div class="profile-bio fake-truncate js-profile-about" style="margin: 0px;">Microfluidics<br /><div class="js-profile-less-about u-linkUnstyled u-tcGrayDarker u-textDecorationUnderline 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id="Pill-react-component-73a315b5-ab2a-4bb1-b168-f5a80a5e4f38"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="42451119" href="https://www.academia.edu/Documents/in/Computational_Fluid_Dynamics_CFD_modelling_and_simulation"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{"color":"gray","children":["Computational Fluid Dynamics (CFD) modelling and simulation"]}" data-trace="false" data-dom-id="Pill-react-component-19335f8a-c531-4792-b189-f0df573b4306"></div> <div id="Pill-react-component-19335f8a-c531-4792-b189-f0df573b4306"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="42451119" href="https://www.academia.edu/Documents/in/Particle-laden_Flow"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{"color":"gray","children":["Particle-laden Flow"]}" data-trace="false" data-dom-id="Pill-react-component-4627baff-52f5-4e6e-896e-f62d417cdaf6"></div> <div id="Pill-react-component-4627baff-52f5-4e6e-896e-f62d417cdaf6"></div> </a></div></div></div></div><div class="right-panel-container"><div class="user-content-wrapper"><div class="uploads-container" id="social-redesign-work-container"><div class="upload-header"><h2 class="ds2-5-heading-sans-serif-xs">Uploads</h2></div><div class="documents-container backbone-social-profile-documents" style="width: 100%;"><div class="u-taCenter"></div><div class="profile--tab_content_container js-tab-pane tab-pane active" id="all"><div class="profile--tab_heading_container js-section-heading" data-section="Papers" id="Papers"><h3 class="profile--tab_heading_container">Papers by Teng Zhou</h3></div><div class="js-work-strip profile--work_container" data-work-id="117239390"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect"><img alt="Research paper thumbnail of An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect">An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect</a></div><div class="wp-workCard_item"><span>Journal of Fluids Engineering-transactions of The Asme</span><span>, May 19, 2015</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Topology optimization method is applied to a contraction–expansion structure, based on which a si...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. The mixing efficiency is further optimized via iterations on key geometric parameters associated with the one-layer mixer designed. Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239390"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239390"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239390; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239390]").text(description); $(".js-view-count[data-work-id=117239390]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239390; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239390']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239390, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239390]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239390,"title":"An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect","translated_title":"","metadata":{"abstract":"Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. The mixing efficiency is further optimized via iterations on key geometric parameters associated with the one-layer mixer designed. Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.","publisher":"ASM International","publication_date":{"day":19,"month":5,"year":2015,"errors":{}},"publication_name":"Journal of Fluids Engineering-transactions of The Asme"},"translated_abstract":"Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. 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Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.","internal_url":"https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect","translated_internal_url":"","created_at":"2024-04-08T11:24:36.942-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":1008960,"name":"Reynolds Number","url":"https://www.academia.edu/Documents/in/Reynolds_Number"}],"urls":[{"id":40944631,"url":"https://doi.org/10.1115/1.4030288"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239389"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239389/Euler_force_actuation_mechanism_for_siphon_valving_in_compact_disk_like_microfluidic_chips"><img alt="Research paper thumbnail of Euler force actuation mechanism for siphon valving in compact disk-like microfluidic chips" class="work-thumbnail" src="https://attachments.academia-assets.com/113148630/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239389/Euler_force_actuation_mechanism_for_siphon_valving_in_compact_disk_like_microfluidic_chips">Euler force actuation mechanism for siphon valving in compact disk-like microfluidic chips</a></div><div class="wp-workCard_item"><span>Biomicrofluidics</span><span>, Mar 1, 2014</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f38dee00431c72bf6e8418c6d30c7ae5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148630,"asset_id":117239389,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148630/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239389"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239389"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239389; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239389]").text(description); $(".js-view-count[data-work-id=117239389]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239389; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239389']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239389, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "f38dee00431c72bf6e8418c6d30c7ae5" } } $('.js-work-strip[data-work-id=117239389]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239389,"title":"Euler force actuation mechanism for siphon valving in compact disk-like microfluidic chips","translated_title":"","metadata":{"publisher":"American Institute of Physics","grobid_abstract":"Based on the Euler force induced by the acceleration of compact disk (CD)-like microfluidic chip, this paper presents a novel actuation mechanism for siphon valving. At the preliminary stage of acceleration, the Euler force in the tangential direction of CD-like chip takes the primary place compared with the centrifugal force to function as the actuation of the flow, which fills the siphon and actuates the siphon valving. The Euler force actuation mechanism is demonstrated by the numerical solution of the phase-field based mathematical model for the flow in siphon valve. In addition, experimental validation is implemented in the polymethylmethacrylate-based CD-like microfluidic chip manufactured using CO 2 laser engraving technique. To prove the application of the proposed Euler force actuation mechanism, whole blood separation and plasma extraction has been conducted using the Euler force actuated siphon valving. The newly introduced actuation mechanism overcomes the dependence on hydrophilic capillary filling of siphon by avoiding external manipulation or surface treatments of polymeric material. The sacrifice for highly integrated processing in pneumatic pumping technique is also prevented by excluding the volume-occupied compressed air chamber. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239387"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity"><img alt="Research paper thumbnail of Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity" class="work-thumbnail" src="https://attachments.academia-assets.com/113148672/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity">Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity</a></div><div class="wp-workCard_item"><span>Computer Methods in Applied Mechanics and Engineering</span><span>, Nov 1, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4d9e2389f1f1365a2d4118dde6d3c6ba" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148672,"asset_id":117239387,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239387"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239387"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239387; 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To meet this purpose, we propose an inverse computational design procedure for the discovery of suitable periodic micro-textures, based on three different tilings of the plane. The symmetric tiles of the lattice are regular triangles, quadrangles, and hexagons. The goal of the inverse design procedure is to achieve the robust Cassie-Baxter state, in which the liquid/vapour interface is mathematically described using the Young-Laplace equation on the lattice, and a topology optimisation approach is utilised to construct a variational problem for the inverse design procedure. Based on numerical calculations of the constructed variational problem, underlying effects are revealed for several factors, including the Bond number, duty ratio, feature size, and lattice constant. The effects of feature size and lattice constant provide approaches for compromisingly considering the robustness of the Cassie-Baxter mode and manufacturability of the inversely designed micro-textures; the effect of the lattice constant permits the scaling properties of the derived patterns, and this in turn provides an approach to avoid the elasto-capillary instability driven collapse of the micro/nanostructures in the derived micro-textures. Further, a monolithic inverse design procedure for the periodic micro-textures is proposed in the conclusions, with synthetically considering the manufacturability as well as contact angle and surface-volume ratio of the liquid bulge held by the supported liquid/vapour interface.","publication_date":{"day":1,"month":11,"year":2018,"errors":{}},"publication_name":"Computer Methods in Applied Mechanics and Engineering","grobid_abstract_attachment_id":113148672},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_internal_url":"","created_at":"2024-04-08T11:24:36.553-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148672,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148672/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420240408-1-ctz7ar.pdf","download_url":"https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148672/j.cma.2018.06.03420240408-1-ctz7ar-libre.pdf?1712605058=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027840\u0026Signature=Yx7Q8DbwqPjTKoYKm4IrueXB7B1ItoInjMrw~0yAvuWZvZGvuMuSicU0x5TTgoBeHFW4j53fP5QSZ4WDtAk-5tzZ4Nt~~kzHUFe2r4qJrzsCYJNtwaP9m-iazDkSl-wo8vIlOfalGuQVB5G5Z0fvpogzLmTq7ui6Vatg2c6XlBgv3P5aMR2XV0QGTNMrSrgBM6VKQMEqfmZFPJT1mcjBtzrB-X5ERdPb4vy4Yx4WKOZ8i7XAFJyzHDV6v~DFi-1wUT4Nac8ePkmOlR7jNo~4wEvyBPCgg5qBhgHFWRsIx0FUY6T3u44O0tTDa2vGl8rUYRCsHctIAvhfjpdH0wxBgQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_slug":"","page_count":23,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148672,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148672/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420240408-1-ctz7ar.pdf","download_url":"https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148672/j.cma.2018.06.03420240408-1-ctz7ar-libre.pdf?1712605058=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027840\u0026Signature=Yx7Q8DbwqPjTKoYKm4IrueXB7B1ItoInjMrw~0yAvuWZvZGvuMuSicU0x5TTgoBeHFW4j53fP5QSZ4WDtAk-5tzZ4Nt~~kzHUFe2r4qJrzsCYJNtwaP9m-iazDkSl-wo8vIlOfalGuQVB5G5Z0fvpogzLmTq7ui6Vatg2c6XlBgv3P5aMR2XV0QGTNMrSrgBM6VKQMEqfmZFPJT1mcjBtzrB-X5ERdPb4vy4Yx4WKOZ8i7XAFJyzHDV6v~DFi-1wUT4Nac8ePkmOlR7jNo~4wEvyBPCgg5qBhgHFWRsIx0FUY6T3u44O0tTDa2vGl8rUYRCsHctIAvhfjpdH0wxBgQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"}],"urls":[{"id":40944628,"url":"https://doi.org/10.1016/j.cma.2018.06.034"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239386"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer"><img alt="Research paper thumbnail of Topology optimization of electrode patterns for electroosmotic micromixer" class="work-thumbnail" src="https://attachments.academia-assets.com/113148673/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer">Topology optimization of electrode patterns for electroosmotic micromixer</a></div><div class="wp-workCard_item"><span>International Journal of Heat and Mass Transfer</span><span>, Nov 1, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="cd2e53cccd605f35e3763e0873db4aae" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148673,"asset_id":117239386,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239386"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239386"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239386; 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The shape and position of electrode pairs, whose induced charges are in contact with the fluid, determine the electric field and hence the resulting fluid-dynamic velocity distribution. In this paper, we address the inverse design of the electrode-pair patterns in such actuation mechanisms. Our approach is to use topology optimization to inversely determine the patterns of an electrode pair. The optimization procedure requires a mathematical description of the desired fluid behaviour, and then drives the patterns of the electrode pairs to achieve the goal performance. We demonstrate the behaviour of the procedure, which couples the Navier-Stokes equations with charge transportation, to implement an efficient electroosmotic micromixer for laminar microflow. We show that the procedure allows to investigate such microflows under the influence of selected parameter variations, thereby exploring the design space towards optimal device performance. This developed method is novel on the topology optimization of a surface structure to control bulk performance and its implementation over a lower-dimensional surface of an otherwise volumetric domain, where the material interpolation is implemented between Dirichlet and Newmann types of boundary conditions.","publication_date":{"day":1,"month":11,"year":2018,"errors":{}},"publication_name":"International Journal of Heat and Mass Transfer","grobid_abstract_attachment_id":113148673},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer","translated_internal_url":"","created_at":"2024-04-08T11:24:36.353-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148673,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148673/thumbnails/1.jpg","file_name":"j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7.pdf","download_url":"https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Topology_optimization_of_electrode_patte.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148673/j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7-libre.pdf?1712605018=\u0026response-content-disposition=attachment%3B+filename%3DTopology_optimization_of_electrode_patte.pdf\u0026Expires=1733027840\u0026Signature=KBmZfbHIFtsdmEi8e6AObdiCq4KLiFctRpqigjHc28EOFLRYRuU5nd62R~P-de0VYkP8FpcWNbvlhqhl1wPW-FOfn0l6A~3vEV4ND8QIwD9BtfnMHdIvOIRlnitLR8E4yqfVq7UasigwUhXiguE9vDArt-ZpO1tgu4QmQzE9bIoMlfmWCar1oHzcuSBIBEUzoFwWODrmKRD3OFn0Q3jDBoLE094vpS7cp41R8uQkCK6L9kStdTFTDi-m3Oss3qNe5PUydZFv6zOyWQvuo9BdmoavQ~~9DznGNnjDzG89veCWeJ9IXVIRv4oR29Teb2SzZ0ALpJofSDfHF7kB~jfmuw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer","translated_slug":"","page_count":17,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148673,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148673/thumbnails/1.jpg","file_name":"j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7.pdf","download_url":"https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Topology_optimization_of_electrode_patte.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148673/j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7-libre.pdf?1712605018=\u0026response-content-disposition=attachment%3B+filename%3DTopology_optimization_of_electrode_patte.pdf\u0026Expires=1733027840\u0026Signature=KBmZfbHIFtsdmEi8e6AObdiCq4KLiFctRpqigjHc28EOFLRYRuU5nd62R~P-de0VYkP8FpcWNbvlhqhl1wPW-FOfn0l6A~3vEV4ND8QIwD9BtfnMHdIvOIRlnitLR8E4yqfVq7UasigwUhXiguE9vDArt-ZpO1tgu4QmQzE9bIoMlfmWCar1oHzcuSBIBEUzoFwWODrmKRD3OFn0Q3jDBoLE094vpS7cp41R8uQkCK6L9kStdTFTDi-m3Oss3qNe5PUydZFv6zOyWQvuo9BdmoavQ~~9DznGNnjDzG89veCWeJ9IXVIRv4oR29Teb2SzZ0ALpJofSDfHF7kB~jfmuw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":20097,"name":"Topology Optimization","url":"https://www.academia.edu/Documents/in/Topology_Optimization"},{"id":33661,"name":"Heat and Mass Transfer","url":"https://www.academia.edu/Documents/in/Heat_and_Mass_Transfer"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":909150,"name":"Electrode","url":"https://www.academia.edu/Documents/in/Electrode"}],"urls":[{"id":40944626,"url":"https://doi.org/10.1016/j.ijheatmasstransfer.2018.06.065"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239384"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip"><img alt="Research paper thumbnail of A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip">A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip</a></div><div class="wp-workCard_item"><span>Modern Physics Letters B</span><span>, Apr 16, 2020</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A transient continuum model of the ODEP chip containing single circular particle inside is constr...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239384"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239384"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239384; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239384]").text(description); $(".js-view-count[data-work-id=117239384]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239384; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239384']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239384, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239384]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239384,"title":"A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip","translated_title":"","metadata":{"abstract":"A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.","publisher":"World Scientific","publication_date":{"day":16,"month":4,"year":2020,"errors":{}},"publication_name":"Modern Physics Letters B"},"translated_abstract":"A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.","internal_url":"https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip","translated_internal_url":"","created_at":"2024-04-08T11:24:36.135-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":27372,"name":"Dielectrophoresis","url":"https://www.academia.edu/Documents/in/Dielectrophoresis"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field"},{"id":2807557,"name":"Maxwell stress tensor","url":"https://www.academia.edu/Documents/in/Maxwell_stress_tensor"}],"urls":[{"id":40944625,"url":"https://doi.org/10.1142/s0217984920502334"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239383"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis"><img alt="Research paper thumbnail of Continuous separation of microparticles based on optically induced dielectrophoresis" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis">Continuous separation of microparticles based on optically induced dielectrophoresis</a></div><div class="wp-workCard_item"><span>Microfluidics and Nanofluidics</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">To achieve high-throughput and high-efficiency separation based on optically induced dielectropho...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239383"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239383"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239383; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239383]").text(description); $(".js-view-count[data-work-id=117239383]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239383; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239383']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239383, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239383]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239383,"title":"Continuous separation of microparticles based on optically induced dielectrophoresis","translated_title":"","metadata":{"abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","publisher":"Springer Science+Business Media","publication_date":{"day":null,"month":null,"year":2022,"errors":{}},"publication_name":"Microfluidics and Nanofluidics"},"translated_abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","internal_url":"https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_internal_url":"","created_at":"2024-04-08T11:24:35.923-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":27372,"name":"Dielectrophoresis","url":"https://www.academia.edu/Documents/in/Dielectrophoresis"},{"id":317912,"name":"Microfluidics and Nanofluidics","url":"https://www.academia.edu/Documents/in/Microfluidics_and_Nanofluidics"},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field"},{"id":3849972,"name":"Springer Nature","url":"https://www.academia.edu/Documents/in/Springer_Nature"}],"urls":[{"id":40944623,"url":"https://doi.org/10.1007/s10404-021-02512-0"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239381"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239381/Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel"><img alt="Research paper thumbnail of Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel" class="work-thumbnail" src="https://attachments.academia-assets.com/113148674/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239381/Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel">Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel</a></div><div class="wp-workCard_item"><span>Electrophoresis</span><span>, Dec 27, 2017</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="01198ce7dc34be42b483cf22bd8e0fd7" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148674,"asset_id":117239381,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148674/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239381"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239381"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239381; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239381]").text(description); $(".js-view-count[data-work-id=117239381]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239381; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239381']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239381, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "01198ce7dc34be42b483cf22bd8e0fd7" } } $('.js-work-strip[data-work-id=117239381]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239381,"title":"Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel","translated_title":"","metadata":{"publisher":"Wiley","grobid_abstract":"The translational motion of small particles in an electrokinetic fluid flow through a constriction can be enhanced by an increase of the applied electric potential. Beyond a critical potential, however, the negative dielectrophoresis (DEP) can overpower other forces to prevent particles that are even smaller than the constriction from passing through the constriction. This DEP choking phenomenon was studied previously for rigid particles. Here, the DEP choking phenomenon is revisited for deformable particles, which are ubiquitous in many biomedical applications. Particle deformability is measured by the particle shear modulus, and the choking conditions are reported through a parametric study that includes the channel geometry, external electric potential, and particle zeta potential. The study was carried out using a numerical model based on an arbitrary Lagrangian-Eulerican (ALE) finite-element method.","publication_date":{"day":27,"month":12,"year":2017,"errors":{}},"publication_name":"Electrophoresis","grobid_abstract_attachment_id":113148674},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239381/Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel","translated_internal_url":"","created_at":"2024-04-08T11:24:35.742-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148674,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148674/thumbnails/1.jpg","file_name":"elps.20170025020240408-1-xrxpj8.pdf","download_url":"https://www.academia.edu/attachments/113148674/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Dielectrophoretic_choking_phenomenon_of.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148674/elps.20170025020240408-1-xrxpj8-libre.pdf?1712605024=\u0026response-content-disposition=attachment%3B+filename%3DDielectrophoretic_choking_phenomenon_of.pdf\u0026Expires=1733027840\u0026Signature=aQvWqNagt2FlRGYw6vPqMGBl~o-RSTNxJ8CoOgSwWhAwVIVBA1~2ZHJYe0zCLmBtpffAAdGFeaUE-zJMlMZbtILBvnSUCfRUTsfYQ1O--lpGYB83fjL3XVonrOG-lUMBMGpIv9aXWeJyypqMD5Duo2fdjw59uL6R2BulPWRDZQbBi~2bToGpf6N~tO69BD8w4Gh6C2DrU-tb8hn~I3isQ70JTWlzRGwSY6Wz8Ypq03N3~RdLKE0E4KFiQG2em2yj8rPIlsEFfTFCZtsUVyX9pg4QVmLtYw54DTBxi2PhhU6tKcDcRFy9txpnEvxUUUteu6VI3g21ei6JHYnNTL-AoA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel","translated_slug":"","page_count":19,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148674,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148674/thumbnails/1.jpg","file_name":"elps.20170025020240408-1-xrxpj8.pdf","download_url":"https://www.academia.edu/attachments/113148674/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Dielectrophoretic_choking_phenomenon_of.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148674/elps.20170025020240408-1-xrxpj8-libre.pdf?1712605024=\u0026response-content-disposition=attachment%3B+filename%3DDielectrophoretic_choking_phenomenon_of.pdf\u0026Expires=1733027840\u0026Signature=aQvWqNagt2FlRGYw6vPqMGBl~o-RSTNxJ8CoOgSwWhAwVIVBA1~2ZHJYe0zCLmBtpffAAdGFeaUE-zJMlMZbtILBvnSUCfRUTsfYQ1O--lpGYB83fjL3XVonrOG-lUMBMGpIv9aXWeJyypqMD5Duo2fdjw59uL6R2BulPWRDZQbBi~2bToGpf6N~tO69BD8w4Gh6C2DrU-tb8hn~I3isQ70JTWlzRGwSY6Wz8Ypq03N3~RdLKE0E4KFiQG2em2yj8rPIlsEFfTFCZtsUVyX9pg4QVmLtYw54DTBxi2PhhU6tKcDcRFy9txpnEvxUUUteu6VI3g21ei6JHYnNTL-AoA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering"},{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":512,"name":"Mechanics","url":"https://www.academia.edu/Documents/in/Mechanics"},{"id":524,"name":"Analytical Chemistry","url":"https://www.academia.edu/Documents/in/Analytical_Chemistry"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":27372,"name":"Dielectrophoresis","url":"https://www.academia.edu/Documents/in/Dielectrophoresis"},{"id":205768,"name":"Electrokinetic Phenomena","url":"https://www.academia.edu/Documents/in/Electrokinetic_Phenomena"},{"id":283531,"name":"Microchannel","url":"https://www.academia.edu/Documents/in/Microchannel"},{"id":371425,"name":"Electrophoresis","url":"https://www.academia.edu/Documents/in/Electrophoresis"},{"id":983062,"name":"Zeta Potential","url":"https://www.academia.edu/Documents/in/Zeta_Potential"},{"id":1681026,"name":"Biochemistry and cell biology","url":"https://www.academia.edu/Documents/in/Biochemistry_and_cell_biology"},{"id":4074029,"name":"Choking","url":"https://www.academia.edu/Documents/in/Choking"}],"urls":[{"id":40944622,"url":"https://doi.org/10.1002/elps.201700250"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239379"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure"><img alt="Research paper thumbnail of An Enhanced Electroosmotic Micromixer with an Efficient Asymmetric Lateral Structure" class="work-thumbnail" src="https://attachments.academia-assets.com/113148620/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure">An Enhanced Electroosmotic Micromixer with an Efficient Asymmetric Lateral Structure</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, Dec 1, 2016</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0c7ea617a5008de962a43db946c08ac1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148620,"asset_id":117239379,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239379"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239379"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239379; 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Here, an efficient electroosmotic micromixer based on a carefully designed lateral structure is demonstrated. The electroosmotic flow in this mixer with an asymmetrical structure induces enhanced disturbance in the micro channel, helping the fluid streams' folding and stretching, thereby enabling appreciable mixing. Quantitative analysis of the mixing efficiency with respect to the potential applied and the flow rate suggests that the electroosmotic microfluidic mixer developed in the present work can achieve efficient mixing with low applied potential.","publication_date":{"day":1,"month":12,"year":2016,"errors":{}},"publication_name":"Micromachines","grobid_abstract_attachment_id":113148620},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure","translated_internal_url":"","created_at":"2024-04-08T11:24:35.565-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148620,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148620/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"An_Enhanced_Electroosmotic_Micromixer_wi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148620/pdf-libre.pdf?1712605022=\u0026response-content-disposition=attachment%3B+filename%3DAn_Enhanced_Electroosmotic_Micromixer_wi.pdf\u0026Expires=1733027840\u0026Signature=b0Ea38tKg~ekB94Gn5zgJ-hgbHzw1dO1vmJNGCCA9R1rF5ohcciVlFguRwGJ3ZIzxTdW~UhHB5p8h--jn2CGvUWbdSDRwytgDmX28VsEyQdPAa6AHiicjC9s2fuXmN2RuiGQlKZnjW0WqWSNaSDQb30jkG7D3euyEVbrZoyKa8uxaevfUNt6A2uia7~GBl6H4x5LYgBMw6DBMehPBqd8RnBOEdTGqQ4sOsbsljKLdaR55VZbo8C93N0VJ1F5uOwXomBONTsyY-LFySC417T4UFq-9re-PnBN7J1Z1p-CsBODlKhs0TsyqaUJlUwzcKIoTZhtQU53cssI-MndU~DBnA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure","translated_slug":"","page_count":8,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148620,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148620/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"An_Enhanced_Electroosmotic_Micromixer_wi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148620/pdf-libre.pdf?1712605022=\u0026response-content-disposition=attachment%3B+filename%3DAn_Enhanced_Electroosmotic_Micromixer_wi.pdf\u0026Expires=1733027840\u0026Signature=b0Ea38tKg~ekB94Gn5zgJ-hgbHzw1dO1vmJNGCCA9R1rF5ohcciVlFguRwGJ3ZIzxTdW~UhHB5p8h--jn2CGvUWbdSDRwytgDmX28VsEyQdPAa6AHiicjC9s2fuXmN2RuiGQlKZnjW0WqWSNaSDQb30jkG7D3euyEVbrZoyKa8uxaevfUNt6A2uia7~GBl6H4x5LYgBMw6DBMehPBqd8RnBOEdTGqQ4sOsbsljKLdaR55VZbo8C93N0VJ1F5uOwXomBONTsyY-LFySC417T4UFq-9re-PnBN7J1Z1p-CsBODlKhs0TsyqaUJlUwzcKIoTZhtQU53cssI-MndU~DBnA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":225478,"name":"Electro-Osmosis","url":"https://www.academia.edu/Documents/in/Electro-Osmosis"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":1008960,"name":"Reynolds Number","url":"https://www.academia.edu/Documents/in/Reynolds_Number"}],"urls":[{"id":40944621,"url":"https://www.mdpi.com/2072-666X/7/12/218/pdf?version=1480598050"}]}, dispatcherData: dispatcherData }); 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By embedding asymmetric electrode arrays on the top and bottom walls of a rectangular microchannel appropriately, the flow perturbations and vortexes can be induced when a DC electric field is imposed. An efficient lateral structure is then sequentially combined with the rectangular microchannel, which enhances the mixing effect significantly. The effects of operational parameters such as the Reynolds number, the applied potential, and the Peclet number on the mixing performance are analyzed in detail by numerical simulations. The results indicate that an enhanced mixing performance can be achieved with low applied potential. The novel method proposed in this paper provides a simple solution for mixing in the field of micro-total-analysis systems.","publication_date":{"day":29,"month":3,"year":2017,"errors":{}},"publication_name":"Micromachines","grobid_abstract_attachment_id":113148622},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239376/A_Novel_Electroosmotic_Micromixer_with_Asymmetric_Lateral_Structures_and_DC_Electrode_Arrays","translated_internal_url":"","created_at":"2024-04-08T11:24:35.193-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148622,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148622/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148622/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_Novel_Electroosmotic_Micromixer_with_A.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148622/pdf-libre.pdf?1712605032=\u0026response-content-disposition=attachment%3B+filename%3DA_Novel_Electroosmotic_Micromixer_with_A.pdf\u0026Expires=1733027840\u0026Signature=E1FG-WJxDU7tHgAgUkyfq7gmf5Cgd~glK~DGw3nfu1cDLOpcVpZVdJjGU9b50T-gZyVIYyQqvV1GygEgT68FbRSX2kBNtAT~dWh7wHd3SsPuHZm0cJJfDXudTBU5NJ2BOQnKHFx7f8Lzj7ZYYCwTt2ULQN0acY3UEgAd0zqavyXZILG9ZHFySqCu8s0sNsxlq~KN5cG8GROgin83u0PrCakkyQ7TP2SuusfYfJP1ZhOOflX96zQQKeuG1gBwna~kQEkdcynunpEMm5Oi-njk6yfiHI3RkrvhlBuTqPW8q7KS9Z8E9D9I73E~hFU9KMxkVejwldhPG050JDctZwkXkw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"A_Novel_Electroosmotic_Micromixer_with_Asymmetric_Lateral_Structures_and_DC_Electrode_Arrays","translated_slug":"","page_count":12,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148622,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148622/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148622/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"A_Novel_Electroosmotic_Micromixer_with_A.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148622/pdf-libre.pdf?1712605032=\u0026response-content-disposition=attachment%3B+filename%3DA_Novel_Electroosmotic_Micromixer_with_A.pdf\u0026Expires=1733027840\u0026Signature=E1FG-WJxDU7tHgAgUkyfq7gmf5Cgd~glK~DGw3nfu1cDLOpcVpZVdJjGU9b50T-gZyVIYyQqvV1GygEgT68FbRSX2kBNtAT~dWh7wHd3SsPuHZm0cJJfDXudTBU5NJ2BOQnKHFx7f8Lzj7ZYYCwTt2ULQN0acY3UEgAd0zqavyXZILG9ZHFySqCu8s0sNsxlq~KN5cG8GROgin83u0PrCakkyQ7TP2SuusfYfJP1ZhOOflX96zQQKeuG1gBwna~kQEkdcynunpEMm5Oi-njk6yfiHI3RkrvhlBuTqPW8q7KS9Z8E9D9I73E~hFU9KMxkVejwldhPG050JDctZwkXkw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":512,"name":"Mechanics","url":"https://www.academia.edu/Documents/in/Mechanics"},{"id":225310,"name":"Vortex","url":"https://www.academia.edu/Documents/in/Vortex"},{"id":283531,"name":"Microchannel","url":"https://www.academia.edu/Documents/in/Microchannel"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":909150,"name":"Electrode","url":"https://www.academia.edu/Documents/in/Electrode"},{"id":1008960,"name":"Reynolds Number","url":"https://www.academia.edu/Documents/in/Reynolds_Number"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field"}],"urls":[{"id":40944618,"url":"https://www.mdpi.com/2072-666X/8/4/105/pdf?version=1490790702"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239375"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239375/Optimal_control_based_inverse_determination_of_electrode_distribution_for_electroosmotic_micromixer"><img alt="Research paper thumbnail of Optimal control-based inverse determination of electrode distribution for electroosmotic micromixer" class="work-thumbnail" src="https://attachments.academia-assets.com/113148619/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239375/Optimal_control_based_inverse_determination_of_electrode_distribution_for_electroosmotic_micromixer">Optimal control-based inverse determination of electrode distribution for electroosmotic micromixer</a></div><div class="wp-workCard_item"><span>arXiv (Cornell University)</span><span>, Dec 31, 2015</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="d8c581802912b1685307a58c5164eb5e" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148619,"asset_id":117239375,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148619/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239375"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239375"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239375; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "d8c581802912b1685307a58c5164eb5e" } } $('.js-work-strip[data-work-id=117239375]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239375,"title":"Optimal control-based inverse determination of electrode distribution for electroosmotic micromixer","translated_title":"","metadata":{"publisher":"Cornell University","grobid_abstract":"This paper presents an optimal control-based inverse method used to determine the distribution of the electrodes for the electroosmotic micromixers with external driven flow from the inlet. 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Numerical results are also provided to demonstrate the effectivity of the proposed method.","publication_date":{"day":31,"month":12,"year":2015,"errors":{}},"publication_name":"arXiv (Cornell University)","grobid_abstract_attachment_id":113148619},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239375/Optimal_control_based_inverse_determination_of_electrode_distribution_for_electroosmotic_micromixer","translated_internal_url":"","created_at":"2024-04-08T11:24:35.002-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148619,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148619/thumbnails/1.jpg","file_name":"1601.pdf","download_url":"https://www.academia.edu/attachments/113148619/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Optimal_control_based_inverse_determinat.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148619/1601-libre.pdf?1712609314=\u0026response-content-disposition=attachment%3B+filename%3DOptimal_control_based_inverse_determinat.pdf\u0026Expires=1733027840\u0026Signature=JV5KMrCA7FWpN8YOTzGpRWRWNYhdGYUDL6L4nJyrtMKjRjTvc4Iut0UDHwJ~j6x-aFOBGcLqbw5t5RuN8F8seaTNfqdoiw9eqOE~fUr~O-g2ISoW9vEIkHDs53RmCfCM7s5k-IGpJL6vUG7iiGASiknATrRED9A6CWESgVDt9P3ph5yWKPt2ObJImcEPkcmBrXVr0GuYI~j5mAO8UJYLpiovD6PEFA8xEk6N97AHvqquWl0hhdt6hVZu9nXquiZxS60WWKdXhsvKsblv7Jgki1AFhgtJsNucESUHzWraXt0UcyMoPd9vcYGrvTUgiRUUAmi9HDaO7RyqSnCMSvYHLw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Optimal_control_based_inverse_determination_of_electrode_distribution_for_electroosmotic_micromixer","translated_slug":"","page_count":13,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148619,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148619/thumbnails/1.jpg","file_name":"1601.pdf","download_url":"https://www.academia.edu/attachments/113148619/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Optimal_control_based_inverse_determinat.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148619/1601-libre.pdf?1712609314=\u0026response-content-disposition=attachment%3B+filename%3DOptimal_control_based_inverse_determinat.pdf\u0026Expires=1733027840\u0026Signature=JV5KMrCA7FWpN8YOTzGpRWRWNYhdGYUDL6L4nJyrtMKjRjTvc4Iut0UDHwJ~j6x-aFOBGcLqbw5t5RuN8F8seaTNfqdoiw9eqOE~fUr~O-g2ISoW9vEIkHDs53RmCfCM7s5k-IGpJL6vUG7iiGASiknATrRED9A6CWESgVDt9P3ph5yWKPt2ObJImcEPkcmBrXVr0GuYI~j5mAO8UJYLpiovD6PEFA8xEk6N97AHvqquWl0hhdt6hVZu9nXquiZxS60WWKdXhsvKsblv7Jgki1AFhgtJsNucESUHzWraXt0UcyMoPd9vcYGrvTUgiRUUAmi9HDaO7RyqSnCMSvYHLw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":113148618,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148618/thumbnails/1.jpg","file_name":"1601.pdf","download_url":"https://www.academia.edu/attachments/113148618/download_file","bulk_download_file_name":"Optimal_control_based_inverse_determinat.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148618/1601-libre.pdf?1712609323=\u0026response-content-disposition=attachment%3B+filename%3DOptimal_control_based_inverse_determinat.pdf\u0026Expires=1733027840\u0026Signature=f6QqtW3GAjz2XvXvMX5esSNjBPxJYQ8VG8Sky-TOfSvAZ4TddwagP79Rd1l0wdMUwnz1TBCrX0arbx~GfmIUSTZ~e8SyWJpGrg1kB0OpVxmdCVwIOH8VfaQiLhOD796N3WDshGKhE7PDNKpU8yiqvilEW3chATsUjGg8ZrceLecJw4QC4bpe6ZoMqWlEYbXWCiaCjfXg7cRT97qWP0ZDaTIaNvViyhlg9eXBVXN~huGly51L-lIlF8Iw3kePNPp0RxUWKhbjr8sAXxotLAMBbtREJdUg0Q0w26OKOsa0v-qeKZiD72tbHs63bq50gYtvCf3HVX8tuzFVJ7~RuD4ZEQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":512,"name":"Mechanics","url":"https://www.academia.edu/Documents/in/Mechanics"},{"id":2200,"name":"Optimal Control","url":"https://www.academia.edu/Documents/in/Optimal_Control"},{"id":893194,"name":"Inverse","url":"https://www.academia.edu/Documents/in/Inverse"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":909150,"name":"Electrode","url":"https://www.academia.edu/Documents/in/Electrode"},{"id":1789645,"name":"Nanoscience and nanotechnology","url":"https://www.academia.edu/Documents/in/Nanoscience_and_nanotechnology-1"}],"urls":[{"id":40944617,"url":"http://arxiv.org/pdf/1601.03076"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239374"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip"><img alt="Research paper thumbnail of Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip" class="work-thumbnail" src="https://attachments.academia-assets.com/113148664/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip">Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip</a></div><div class="wp-workCard_item"><span>Frontiers in Chemistry</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testi...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1f0f6d37c7c4af84cd1520282c6aa2a4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148664,"asset_id":117239374,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239374"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239374"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239374; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239374]").text(description); $(".js-view-count[data-work-id=117239374]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239374; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239374']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239374, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "1f0f6d37c7c4af84cd1520282c6aa2a4" } } $('.js-work-strip[data-work-id=117239374]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239374,"title":"Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip","translated_title":"","metadata":{"abstract":"Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.","publisher":"Frontiers Media SA","ai_title_tag":"Multiplex Cardiac Marker Detection with Snail-Shaped Chip","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Frontiers in Chemistry"},"translated_abstract":"Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.","internal_url":"https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip","translated_internal_url":"","created_at":"2024-04-08T11:24:34.821-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148664,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148664/thumbnails/1.jpg","file_name":"fchem-09-741058.pdf","download_url":"https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Point_of_Care_Testing_for_Multiple_Cardi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148664/fchem-09-741058-libre.pdf?1712605017=\u0026response-content-disposition=attachment%3B+filename%3DPoint_of_Care_Testing_for_Multiple_Cardi.pdf\u0026Expires=1733027840\u0026Signature=dGqw9fFDg598JhPwrIf9N3D~fXQhpNsQ066~1YiBehpNWfIZWBSxoIPxOvECDDAzaitKW5T19OrP0JsGdbR6dzqj32hrG8T7ormLLfRNYAUwbOxCwz9XzDu51UYGmqG8XFiG5r1~4F-u9p~dM3Q-yHNQ09Gbvgx8wv9cuLK6zgUedoWYclNbPIIrNRgXokDuXFy~QSb0nxMCIyms8Qq0gP~F0dQoQm~0UENqaX-5oPTeqsF2YtT0GiTAXIWWZHmXbGVmow2f~HinaTpGn4Uc8Ya6z424reO1YxU8krcq-5qGzTA2NRR9RWuwS7Tn0Nq1aGdJlIO7oLlQ7aVgaxDwvQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip","translated_slug":"","page_count":11,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148664,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148664/thumbnails/1.jpg","file_name":"fchem-09-741058.pdf","download_url":"https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Point_of_Care_Testing_for_Multiple_Cardi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148664/fchem-09-741058-libre.pdf?1712605017=\u0026response-content-disposition=attachment%3B+filename%3DPoint_of_Care_Testing_for_Multiple_Cardi.pdf\u0026Expires=1733027840\u0026Signature=dGqw9fFDg598JhPwrIf9N3D~fXQhpNsQ066~1YiBehpNWfIZWBSxoIPxOvECDDAzaitKW5T19OrP0JsGdbR6dzqj32hrG8T7ormLLfRNYAUwbOxCwz9XzDu51UYGmqG8XFiG5r1~4F-u9p~dM3Q-yHNQ09Gbvgx8wv9cuLK6zgUedoWYclNbPIIrNRgXokDuXFy~QSb0nxMCIyms8Qq0gP~F0dQoQm~0UENqaX-5oPTeqsF2YtT0GiTAXIWWZHmXbGVmow2f~HinaTpGn4Uc8Ya6z424reO1YxU8krcq-5qGzTA2NRR9RWuwS7Tn0Nq1aGdJlIO7oLlQ7aVgaxDwvQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":914941,"name":"Point of Care Testing","url":"https://www.academia.edu/Documents/in/Point_of_Care_Testing"}],"urls":[{"id":40944616,"url":"https://www.frontiersin.org/articles/10.3389/fchem.2021.741058/full"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239373"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239373/Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion"><img alt="Research paper thumbnail of Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion" class="work-thumbnail" src="https://attachments.academia-assets.com/113148617/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239373/Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion">Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion</a></div><div class="wp-workCard_item"><span>National Science Review</span><span>, 2020</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting c...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting clean and sustainable osmotic energy existing in the salinity gradient. However, the current designs of membranes cannot cope with the high output power density and robustness. Here, we construct a sulfonated poly (ether ether ketone) (SPEEK) nanochannel membrane with numerous nanochannels for a membrane-based osmotic power generator. The parallel nanochannels with high space charges show excellent cation-selectivity, which could further be improved by adjusting the length and charge density of nanochannels. Based on numerical simulation, the system with space charge shows better conductivity and selectivity than those of a surface-charged nanochannel. The output power density of our proposed membrane-based device reaches up to 5.8 W/m2 by mixing artificial seawater and river water. Additionally, the SPEEK membranes exhibit good mechanical properties, endowing the possibility of creating ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ffd518629692aa93c622c80c223c51f5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148617,"asset_id":117239373,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148617/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239373"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239373"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239373; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239373]").text(description); $(".js-view-count[data-work-id=117239373]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239373; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239373']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239373, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "ffd518629692aa93c622c80c223c51f5" } } $('.js-work-strip[data-work-id=117239373]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239373,"title":"Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion","translated_title":"","metadata":{"abstract":"The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting clean and sustainable osmotic energy existing in the salinity gradient. However, the current designs of membranes cannot cope with the high output power density and robustness. Here, we construct a sulfonated poly (ether ether ketone) (SPEEK) nanochannel membrane with numerous nanochannels for a membrane-based osmotic power generator. The parallel nanochannels with high space charges show excellent cation-selectivity, which could further be improved by adjusting the length and charge density of nanochannels. Based on numerical simulation, the system with space charge shows better conductivity and selectivity than those of a surface-charged nanochannel. The output power density of our proposed membrane-based device reaches up to 5.8 W/m2 by mixing artificial seawater and river water. Additionally, the SPEEK membranes exhibit good mechanical properties, endowing the possibility of creating ...","publisher":"Oxford University Press (OUP)","publication_date":{"day":null,"month":null,"year":2020,"errors":{}},"publication_name":"National Science Review"},"translated_abstract":"The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting clean and sustainable osmotic energy existing in the salinity gradient. However, the current designs of membranes cannot cope with the high output power density and robustness. Here, we construct a sulfonated poly (ether ether ketone) (SPEEK) nanochannel membrane with numerous nanochannels for a membrane-based osmotic power generator. The parallel nanochannels with high space charges show excellent cation-selectivity, which could further be improved by adjusting the length and charge density of nanochannels. Based on numerical simulation, the system with space charge shows better conductivity and selectivity than those of a surface-charged nanochannel. The output power density of our proposed membrane-based device reaches up to 5.8 W/m2 by mixing artificial seawater and river water. Additionally, the SPEEK membranes exhibit good mechanical properties, endowing the possibility of creating ...","internal_url":"https://www.academia.edu/117239373/Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion","translated_internal_url":"","created_at":"2024-04-08T11:24:34.638-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148617,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148617/thumbnails/1.jpg","file_name":"nwaa057.pdf","download_url":"https://www.academia.edu/attachments/113148617/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Robust_sulfonated_poly_ether_ether_keton.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148617/nwaa057-libre.pdf?1712609303=\u0026response-content-disposition=attachment%3B+filename%3DRobust_sulfonated_poly_ether_ether_keton.pdf\u0026Expires=1733027840\u0026Signature=P6xe1Tu9gJW23ELsYQLSxa8kxVL3ZUETsSv-RmNLPsALodyVh~-TxeQyCxTI59eFtoArv793FpR7t~TB7ipk6z7~oX2ZA5yMCKFjs3C4x3qBsYH2SvDSOrMshLtNxbHG1G7PACDf5EGsoDNG~glD0VHS8Q1M~JcbOraXW9X3bvGHNHsbG1w3NMc1f-gfDNb1MnZhD2QthO1ZRWGXUzSUW0wPa4DBnPyGaxxqnNNMevopz5UHuJ5KNPQaTflYRZJ0KS0gZRQMQC4K1pwKEaajxChf-K0u6GR4axO6zsIDU5WSkK-k5AGapmS4kJ5P2Ised-Xwj734oswvkd2IRe8ECg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion","translated_slug":"","page_count":11,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148617,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148617/thumbnails/1.jpg","file_name":"nwaa057.pdf","download_url":"https://www.academia.edu/attachments/113148617/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Robust_sulfonated_poly_ether_ether_keton.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148617/nwaa057-libre.pdf?1712609303=\u0026response-content-disposition=attachment%3B+filename%3DRobust_sulfonated_poly_ether_ether_keton.pdf\u0026Expires=1733027840\u0026Signature=P6xe1Tu9gJW23ELsYQLSxa8kxVL3ZUETsSv-RmNLPsALodyVh~-TxeQyCxTI59eFtoArv793FpR7t~TB7ipk6z7~oX2ZA5yMCKFjs3C4x3qBsYH2SvDSOrMshLtNxbHG1G7PACDf5EGsoDNG~glD0VHS8Q1M~JcbOraXW9X3bvGHNHsbG1w3NMc1f-gfDNb1MnZhD2QthO1ZRWGXUzSUW0wPa4DBnPyGaxxqnNNMevopz5UHuJ5KNPQaTflYRZJ0KS0gZRQMQC4K1pwKEaajxChf-K0u6GR4axO6zsIDU5WSkK-k5AGapmS4kJ5P2Ised-Xwj734oswvkd2IRe8ECg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":113148616,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148616/thumbnails/1.jpg","file_name":"nwaa057.pdf","download_url":"https://www.academia.edu/attachments/113148616/download_file","bulk_download_file_name":"Robust_sulfonated_poly_ether_ether_keton.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148616/nwaa057-libre.pdf?1712609305=\u0026response-content-disposition=attachment%3B+filename%3DRobust_sulfonated_poly_ether_ether_keton.pdf\u0026Expires=1733027840\u0026Signature=Xx4oudsPH56JAFRGN6nnp2HRmsYqk3k5i-x8gMVMcd62IEy99kLa0xtMxRu2gfYQrDZe2waXmbIb9a3WOjfkzlWqfdDs68cGAg2DCj9lhufbDb9DbukuyDBC3~98B-H8zbWyqpryb9r5QB0tRzGmcGXGfitro3s3V9YFNTrtbOfCfnc-YlN9AapZycGoXSeUV5TjMI4W3PRn4EawvRGOvJuHMuCHCo-5GGv~Ap8kjrst3cO9DGdj-eTl1UdSmUvxPGsBvGbq2evnvGPWhK9k~q7o62uMSP-b6lkZII3vlW31e0oBOLf4eADy59xF8eg1zwLqKig7fJL7vJZ3uSaqOQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":72,"name":"Chemical Engineering","url":"https://www.academia.edu/Documents/in/Chemical_Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":6779,"name":"Science","url":"https://www.academia.edu/Documents/in/Science"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":99631,"name":"Pressure Retarded Osmosis","url":"https://www.academia.edu/Documents/in/Pressure_Retarded_Osmosis"},{"id":111976,"name":"Osmotic power","url":"https://www.academia.edu/Documents/in/Osmotic_power"},{"id":242298,"name":"Membrane","url":"https://www.academia.edu/Documents/in/Membrane"},{"id":2254453,"name":"Power Density","url":"https://www.academia.edu/Documents/in/Power_Density"}],"urls":[{"id":40944615,"url":"http://academic.oup.com/nsr/advance-article-pdf/doi/10.1093/nsr/nwaa057/32990731/nwaa057.pdf"}]}, dispatcherData: dispatcherData }); 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The layout of channel networks can be rather simple, with constant width, straight channels, or the layout can be very complex, with multiple splitters, combiners, or even multiple layers. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="100626520"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/100626520/Combustion_Characteristics_of_Small_Laminar_Flames_in_an_Upward_Decreasing_Magnetic_Field"><img alt="Research paper thumbnail of Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field" class="work-thumbnail" src="https://attachments.academia-assets.com/101395892/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626520/Combustion_Characteristics_of_Small_Laminar_Flames_in_an_Upward_Decreasing_Magnetic_Field">Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field</a></div><div class="wp-workCard_item"><span>Energies</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1a468d1fbd581995a410a0edc333e9a8" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395892,"asset_id":100626520,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395892/download_file?st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626520"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626520"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626520; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=100626520]").text(description); $(".js-view-count[data-work-id=100626520]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 100626520; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='100626520']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 100626520, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "1a468d1fbd581995a410a0edc333e9a8" } } $('.js-work-strip[data-work-id=100626520]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":100626520,"title":"Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field","translated_title":"","metadata":{"abstract":"The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of ...","publisher":"MDPI AG","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Energies"},"translated_abstract":"The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of 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src="https://attachments.academia-assets.com/101395891/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626519/Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions">Enzyme Method-Based Microfluidic Chip for the Rapid Detection of Copper Ions</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Metal ions in high concentrations can pollute the marine environment. Human activities and indust...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5e20507e3a59f59594fd639605e9f2a4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395891,"asset_id":100626519,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626519; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=100626519]").text(description); $(".js-view-count[data-work-id=100626519]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 100626519; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='100626519']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 100626519, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "5e20507e3a59f59594fd639605e9f2a4" } } $('.js-work-strip[data-work-id=100626519]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":100626519,"title":"Enzyme Method-Based Microfluidic Chip for the Rapid Detection of Copper Ions","translated_title":"","metadata":{"abstract":"Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...","publisher":"MDPI AG","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Micromachines"},"translated_abstract":"Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...","internal_url":"https://www.academia.edu/100626519/Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions","translated_internal_url":"","created_at":"2023-04-23T07:09:30.901-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":101395891,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395891/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395891/pdf-libre.pdf?1682280149=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Cv08s3KkiwZ9mDDK50nH5xYaa6UDaPQ5oaT4WTuNhdfRURGADkx8Uw87keqp45S-V1I0czFJwkj0JzZYq7uPDG4fBenLYlS4GOvati4u-VQJnPGkzRFOLdjp9JA6s8Ei9ffm~2pTog6fw1a~I9E96ELFUVpwLkCO2Ztj5~1wYZ2rdMnDTZJ7tN5QSO5RGl1bTOwxS8fX9sRcI6uR9CLXvxry0tBYxOvyM1-4Ahg5cvAftyU1lf4eGt4f4l~dKknm09M5Vo3nEDu4MXTjSYwsj9fNJDXegfKygPecGJG3iw3f8GDyqd83M4wFKfpJ8vpKT4Mtq8daWtCj~8GYLllRCQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions","translated_slug":"","page_count":10,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":101395891,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395891/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395891/pdf-libre.pdf?1682280149=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Cv08s3KkiwZ9mDDK50nH5xYaa6UDaPQ5oaT4WTuNhdfRURGADkx8Uw87keqp45S-V1I0czFJwkj0JzZYq7uPDG4fBenLYlS4GOvati4u-VQJnPGkzRFOLdjp9JA6s8Ei9ffm~2pTog6fw1a~I9E96ELFUVpwLkCO2Ztj5~1wYZ2rdMnDTZJ7tN5QSO5RGl1bTOwxS8fX9sRcI6uR9CLXvxry0tBYxOvyM1-4Ahg5cvAftyU1lf4eGt4f4l~dKknm09M5Vo3nEDu4MXTjSYwsj9fNJDXegfKygPecGJG3iw3f8GDyqd83M4wFKfpJ8vpKT4Mtq8daWtCj~8GYLllRCQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":101395890,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395890/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395890/download_file","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395890/pdf-libre.pdf?1682280152=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Zz93gQY02LnYKwmM10RseTcM~SYe-CQaDUfdibIBuRYMXm-rU2599s1kjhF3bB~ktfwWTZhwTXiwNWawJdmr2ZT5rQkDgQmYz2zN0SM7yOxVv~v26rB4pQ23qISgNHPbarDNQbqGaTcFG4fLpxSjBUjVH0MgLvDa0-Kh~oYZD2P93qARmmwmRPUbctvsn~gGjKYL8lfPU~OViWTN1--SxDMlb3UVC4e-Kuqnitc0ba0inVoUe1CxoMNB-4vbclprpcgaogFbeuoRDesyHphPjyKhuMzKSAc4Za4~-6Mxr8Gx30bgSQX2wW-OOwvfMFB-9u0jf9c~k1WEy6VS-suIIQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":80692,"name":"Copper","url":"https://www.academia.edu/Documents/in/Copper"},{"id":184467,"name":"Seawater","url":"https://www.academia.edu/Documents/in/Seawater"},{"id":322954,"name":"Chip","url":"https://www.academia.edu/Documents/in/Chip"},{"id":753116,"name":"Absorbance","url":"https://www.academia.edu/Documents/in/Absorbance"},{"id":2465388,"name":"Naked Eye","url":"https://www.academia.edu/Documents/in/Naked_Eye"}],"urls":[{"id":30849374,"url":"https://www.mdpi.com/2072-666X/12/11/1380/pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="100626518"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity"><img alt="Research paper thumbnail of Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity" class="work-thumbnail" src="https://attachments.academia-assets.com/101395918/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity">Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity</a></div><div class="wp-workCard_item"><span>Computer Methods in Applied Mechanics and Engineering</span><span>, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b52599d72a820fafff221a89b61abb82" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395918,"asset_id":100626518,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626518"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626518"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626518; 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To meet this purpose, we propose an inverse computational design procedure for the discovery of suitable periodic micro-textures, based on three different tilings of the plane. The symmetric tiles of the lattice are regular triangles, quadrangles, and hexagons. The goal of the inverse design procedure is to achieve the robust Cassie-Baxter state, in which the liquid/vapour interface is mathematically described using the Young-Laplace equation on the lattice, and a topology optimisation approach is utilised to construct a variational problem for the inverse design procedure. Based on numerical calculations of the constructed variational problem, underlying effects are revealed for several factors, including the Bond number, duty ratio, feature size, and lattice constant. The effects of feature size and lattice constant provide approaches for compromisingly considering the robustness of the Cassie-Baxter mode and manufacturability of the inversely designed micro-textures; the effect of the lattice constant permits the scaling properties of the derived patterns, and this in turn provides an approach to avoid the elasto-capillary instability driven collapse of the micro/nanostructures in the derived micro-textures. Further, a monolithic inverse design procedure for the periodic micro-textures is proposed in the conclusions, with synthetically considering the manufacturability as well as contact angle and surface-volume ratio of the liquid bulge held by the supported liquid/vapour interface.","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Computer Methods in Applied Mechanics and Engineering","grobid_abstract_attachment_id":101395918},"translated_abstract":null,"internal_url":"https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_internal_url":"","created_at":"2023-04-23T07:09:30.731-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":101395918,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395918/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420230423-1-ia3as3.pdf","download_url":"https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395918/j.cma.2018.06.03420230423-1-ia3as3-libre.pdf?1682280490=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027841\u0026Signature=a4JCfXHOeIjDCrkeJ0FCYs9bbNnGl4Zq168b0PNuHlVhYhfyFpbZbJRACpSmOKj-ZM3ARnH5CByWQpsRRINy0IpHQkLERcNMTnna0Er3jlG3nt3kvZYMxEK22lwLJ4x8Bs3~WcmbnPFD9CztsPEAdN2BJT~VytvD6R78Ds0aZy2WDLh4-ClvvXGgBSn8OIGLS~ZDBx1J-fUe-fhZFAu4OXDJuuJx6K8OSSuzoy3oZ1b4qMKKt9veE8MOHsDE61ghd4gDr3A0P2Y60wsL0otupnX6msbMImpRdPgcQlzwbFNGt9ZXywT7Ix0ZVcT5tG9R0ouD9mpzt83qeGraGu8Vig__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_slug":"","page_count":23,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":101395918,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395918/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420230423-1-ia3as3.pdf","download_url":"https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395918/j.cma.2018.06.03420230423-1-ia3as3-libre.pdf?1682280490=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027841\u0026Signature=a4JCfXHOeIjDCrkeJ0FCYs9bbNnGl4Zq168b0PNuHlVhYhfyFpbZbJRACpSmOKj-ZM3ARnH5CByWQpsRRINy0IpHQkLERcNMTnna0Er3jlG3nt3kvZYMxEK22lwLJ4x8Bs3~WcmbnPFD9CztsPEAdN2BJT~VytvD6R78Ds0aZy2WDLh4-ClvvXGgBSn8OIGLS~ZDBx1J-fUe-fhZFAu4OXDJuuJx6K8OSSuzoy3oZ1b4qMKKt9veE8MOHsDE61ghd4gDr3A0P2Y60wsL0otupnX6msbMImpRdPgcQlzwbFNGt9ZXywT7Ix0ZVcT5tG9R0ouD9mpzt83qeGraGu8Vig__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"}],"urls":[{"id":30849373,"url":"https://api.elsevier.com/content/article/PII:S0045782518303323?httpAccept=text/xml"}]}, dispatcherData: dispatcherData }); 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window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76752476]").text(description); $(".js-view-count[data-work-id=76752476]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76752476; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76752476']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76752476, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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Although both potential and pH gradient can significantly change the performance of ion current rectification in nanoscale, the potential mechanism is still not fully understood. In this study, the ion current rectification, surface charge distribution and ion selectivity of silica nanopore under different background salt concentration and pH gradient were discussed by an analytical model, which takes into account the effects of electroosmotic flow, multiple ionic species, and the acid base neutralization. The results show that the polarity of nanopore rectifier can be changed by changing the acidity and alkalinity at both ends of the nanopore. For the first time, we find that the rectification polarity of silica conical nanopore exhibits different performances under high and low electric field intensity. One case in this study shows the rectification ratio curve of the nanopore will have a maximum or minimum value and the extreme point is near the zero of the ion current. With the increase of the concentration of background salt solution, the voltage at the zero point of ion current approaches the zero point, and then the maximum or minimum point moves to the left. The extreme point offset and polarity reversal phenomena may have potential application value in nanopore-based sensing devices.","publication_date":{"day":null,"month":null,"year":2020,"errors":{}},"publication_name":"SN Applied Sciences","grobid_abstract_attachment_id":84351649},"translated_abstract":null,"internal_url":"https://www.academia.edu/76752476/The_polarization_reverse_of_diode_like_conical_nanopore_under_pH_gradient","translated_internal_url":"","created_at":"2022-04-17T16:37:23.635-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":84351649,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351649/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351649/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351649/s42452-020-03675-1-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=TrQBeIN5o2P57Womyo~Rrz5Ct60SsyMuVIq8D5ythld69jyvEdBMJ8USPDtF8KjKZL30FWLzXa9E~r9WpURol0ANNGgfvzhTlh9ILH1bxRtTLux1WDFXe7KEe4YalTnV3~m90h8chgBc6mZdJumbP1Ro3Ug-LpNQLCEOF7xPZaX3aiSRdwJisWJfLUH~zg5L4edElEdOm1nUAnexuji46n2AWcAwhmZvBap4FkkdLt8Y~y2QLYX0dIGrDRtTW~PP7rSEy1WiqmzDObvug20KnCfu6jVZAILWQmddIJVDsYWkPgVleS5euWx9YzKfJ-QAISmksa7hltmqzp~cF4LSrA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"The_polarization_reverse_of_diode_like_conical_nanopore_under_pH_gradient","translated_slug":"","page_count":14,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":84351649,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351649/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351649/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351649/s42452-020-03675-1-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=TrQBeIN5o2P57Womyo~Rrz5Ct60SsyMuVIq8D5ythld69jyvEdBMJ8USPDtF8KjKZL30FWLzXa9E~r9WpURol0ANNGgfvzhTlh9ILH1bxRtTLux1WDFXe7KEe4YalTnV3~m90h8chgBc6mZdJumbP1Ro3Ug-LpNQLCEOF7xPZaX3aiSRdwJisWJfLUH~zg5L4edElEdOm1nUAnexuji46n2AWcAwhmZvBap4FkkdLt8Y~y2QLYX0dIGrDRtTW~PP7rSEy1WiqmzDObvug20KnCfu6jVZAILWQmddIJVDsYWkPgVleS5euWx9YzKfJ-QAISmksa7hltmqzp~cF4LSrA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":84351650,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351650/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351650/download_file","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351650/s42452-020-03675-1-libre.pdf?1650239167=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=MFSQp2pyl81D6S1771KrZ~50WhSSF9qir44t3XHsOl0iFMVarvT0nyLKBDZyyjEHl~GxCRmOApF1Rvl4lW5pKg-ShzoiKojCLaoWW0p-7ir-WEv4g6aoQ~zswRbq7RVZVs6PDmvL-R9ach~1lX2Smmc3eCsS2iy-QMBcgfJmAy4z1vGLz1YhF6yMS1~aUCgDrJ0cNM4dqC4hX~~Kty4oWEW0~MGtTUDCpFOKUW6Jft4KA2hK70UpFj918TNy1dK0xjb9tnh~m2DKsUj4ic7lU~wKSBPYlKylvVUYzM0PTaWYivjXibz-w4aNHmIRWcRP1HomkHqiVzSuDxiUnlcozQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"}],"urls":[{"id":19595376,"url":"http://link.springer.com/content/pdf/10.1007/s42452-020-03675-1.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="76752475"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis"><img alt="Research paper thumbnail of Continuous separation of microparticles based on optically induced dielectrophoresis" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis">Continuous separation of microparticles based on optically induced dielectrophoresis</a></div><div class="wp-workCard_item"><span>Microfluidics and Nanofluidics</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">To achieve high-throughput and high-efficiency separation based on optically induced dielectropho...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="76752475"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="76752475"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76752475; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76752475]").text(description); $(".js-view-count[data-work-id=76752475]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76752475; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76752475']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76752475, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=76752475]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76752475,"title":"Continuous separation of microparticles based on optically induced dielectrophoresis","translated_title":"","metadata":{"abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","publisher":"Springer Science and Business Media LLC","publication_date":{"day":null,"month":null,"year":2022,"errors":{}},"publication_name":"Microfluidics and Nanofluidics"},"translated_abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","internal_url":"https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_internal_url":"","created_at":"2022-04-17T16:37:23.492-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":317912,"name":"Microfluidics and Nanofluidics","url":"https://www.academia.edu/Documents/in/Microfluidics_and_Nanofluidics"},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering"},{"id":3849972,"name":"Springer Nature","url":"https://www.academia.edu/Documents/in/Springer_Nature"}],"urls":[{"id":19595375,"url":"https://link.springer.com/content/pdf/10.1007/s10404-021-02512-0.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="76752474"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/76752474/Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis"><img alt="Research paper thumbnail of Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis" class="work-thumbnail" src="https://attachments.academia-assets.com/84351648/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/76752474/Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis">Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on li...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. The current micromixer provides a favorable fluid-mixing method based on an optical virtual electrode, and could promote...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="7eead9f4feabe0fbf281e9fb7cce84ba" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84351648,"asset_id":76752474,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84351648/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="76752474"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="76752474"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76752474; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76752474]").text(description); $(".js-view-count[data-work-id=76752474]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76752474; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76752474']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76752474, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "7eead9f4feabe0fbf281e9fb7cce84ba" } } $('.js-work-strip[data-work-id=76752474]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76752474,"title":"Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis","translated_title":"","metadata":{"abstract":"In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. The current micromixer provides a favorable fluid-mixing method based on an optical virtual electrode, and could promote...","publisher":"Micromachines","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Micromachines"},"translated_abstract":"In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="4521295" id="papers"><div class="js-work-strip profile--work_container" data-work-id="117239390"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect"><img alt="Research paper thumbnail of An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect">An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect</a></div><div class="wp-workCard_item"><span>Journal of Fluids Engineering-transactions of The Asme</span><span>, May 19, 2015</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Topology optimization method is applied to a contraction–expansion structure, based on which a si...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. The mixing efficiency is further optimized via iterations on key geometric parameters associated with the one-layer mixer designed. Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239390"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239390"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239390; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239390]").text(description); $(".js-view-count[data-work-id=117239390]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239390; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239390']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239390, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239390]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239390,"title":"An Enhanced One-Layer Passive Microfluidic Mixer With an Optimized Lateral Structure With the Dean Effect","translated_title":"","metadata":{"abstract":"Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. The mixing efficiency is further optimized via iterations on key geometric parameters associated with the one-layer mixer designed. Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.","publisher":"ASM International","publication_date":{"day":19,"month":5,"year":2015,"errors":{}},"publication_name":"Journal of Fluids Engineering-transactions of The Asme"},"translated_abstract":"Topology optimization method is applied to a contraction–expansion structure, based on which a simplified lateral flow structure is generated using the Boolean operation. A new one-layer mixer is then designed by sequentially connecting this lateral structure and bent channels. The mixing efficiency is further optimized via iterations on key geometric parameters associated with the one-layer mixer designed. Numerical results indicate that the optimized mixer has better mixing efficiency than the conventional contraction–expansion mixer for a wide range of the Reynolds number.","internal_url":"https://www.academia.edu/117239390/An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect","translated_internal_url":"","created_at":"2024-04-08T11:24:36.942-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"An_Enhanced_One_Layer_Passive_Microfluidic_Mixer_With_an_Optimized_Lateral_Structure_With_the_Dean_Effect","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":1008960,"name":"Reynolds Number","url":"https://www.academia.edu/Documents/in/Reynolds_Number"}],"urls":[{"id":40944631,"url":"https://doi.org/10.1115/1.4030288"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239389"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239389/Euler_force_actuation_mechanism_for_siphon_valving_in_compact_disk_like_microfluidic_chips"><img alt="Research paper thumbnail of Euler force actuation mechanism for siphon valving in compact disk-like microfluidic chips" class="work-thumbnail" src="https://attachments.academia-assets.com/113148630/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239389/Euler_force_actuation_mechanism_for_siphon_valving_in_compact_disk_like_microfluidic_chips">Euler force actuation mechanism for siphon valving in compact disk-like microfluidic chips</a></div><div class="wp-workCard_item"><span>Biomicrofluidics</span><span>, Mar 1, 2014</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f38dee00431c72bf6e8418c6d30c7ae5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148630,"asset_id":117239389,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148630/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239389"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239389"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239389; 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At the preliminary stage of acceleration, the Euler force in the tangential direction of CD-like chip takes the primary place compared with the centrifugal force to function as the actuation of the flow, which fills the siphon and actuates the siphon valving. The Euler force actuation mechanism is demonstrated by the numerical solution of the phase-field based mathematical model for the flow in siphon valve. In addition, experimental validation is implemented in the polymethylmethacrylate-based CD-like microfluidic chip manufactured using CO 2 laser engraving technique. To prove the application of the proposed Euler force actuation mechanism, whole blood separation and plasma extraction has been conducted using the Euler force actuated siphon valving. The newly introduced actuation mechanism overcomes the dependence on hydrophilic capillary filling of siphon by avoiding external manipulation or surface treatments of polymeric material. The sacrifice for highly integrated processing in pneumatic pumping technique is also prevented by excluding the volume-occupied compressed air chamber. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239387"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity"><img alt="Research paper thumbnail of Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity" class="work-thumbnail" src="https://attachments.academia-assets.com/113148672/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity">Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity</a></div><div class="wp-workCard_item"><span>Computer Methods in Applied Mechanics and Engineering</span><span>, Nov 1, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4d9e2389f1f1365a2d4118dde6d3c6ba" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148672,"asset_id":117239387,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239387"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239387"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239387; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239387]").text(description); $(".js-view-count[data-work-id=117239387]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239387; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239387']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239387, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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To meet this purpose, we propose an inverse computational design procedure for the discovery of suitable periodic micro-textures, based on three different tilings of the plane. The symmetric tiles of the lattice are regular triangles, quadrangles, and hexagons. The goal of the inverse design procedure is to achieve the robust Cassie-Baxter state, in which the liquid/vapour interface is mathematically described using the Young-Laplace equation on the lattice, and a topology optimisation approach is utilised to construct a variational problem for the inverse design procedure. Based on numerical calculations of the constructed variational problem, underlying effects are revealed for several factors, including the Bond number, duty ratio, feature size, and lattice constant. The effects of feature size and lattice constant provide approaches for compromisingly considering the robustness of the Cassie-Baxter mode and manufacturability of the inversely designed micro-textures; the effect of the lattice constant permits the scaling properties of the derived patterns, and this in turn provides an approach to avoid the elasto-capillary instability driven collapse of the micro/nanostructures in the derived micro-textures. Further, a monolithic inverse design procedure for the periodic micro-textures is proposed in the conclusions, with synthetically considering the manufacturability as well as contact angle and surface-volume ratio of the liquid bulge held by the supported liquid/vapour interface.","publication_date":{"day":1,"month":11,"year":2018,"errors":{}},"publication_name":"Computer Methods in Applied Mechanics and Engineering","grobid_abstract_attachment_id":113148672},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239387/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_internal_url":"","created_at":"2024-04-08T11:24:36.553-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148672,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148672/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420240408-1-ctz7ar.pdf","download_url":"https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148672/j.cma.2018.06.03420240408-1-ctz7ar-libre.pdf?1712605058=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027840\u0026Signature=Yx7Q8DbwqPjTKoYKm4IrueXB7B1ItoInjMrw~0yAvuWZvZGvuMuSicU0x5TTgoBeHFW4j53fP5QSZ4WDtAk-5tzZ4Nt~~kzHUFe2r4qJrzsCYJNtwaP9m-iazDkSl-wo8vIlOfalGuQVB5G5Z0fvpogzLmTq7ui6Vatg2c6XlBgv3P5aMR2XV0QGTNMrSrgBM6VKQMEqfmZFPJT1mcjBtzrB-X5ERdPb4vy4Yx4WKOZ8i7XAFJyzHDV6v~DFi-1wUT4Nac8ePkmOlR7jNo~4wEvyBPCgg5qBhgHFWRsIx0FUY6T3u44O0tTDa2vGl8rUYRCsHctIAvhfjpdH0wxBgQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_slug":"","page_count":23,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148672,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148672/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420240408-1-ctz7ar.pdf","download_url":"https://www.academia.edu/attachments/113148672/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148672/j.cma.2018.06.03420240408-1-ctz7ar-libre.pdf?1712605058=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027840\u0026Signature=Yx7Q8DbwqPjTKoYKm4IrueXB7B1ItoInjMrw~0yAvuWZvZGvuMuSicU0x5TTgoBeHFW4j53fP5QSZ4WDtAk-5tzZ4Nt~~kzHUFe2r4qJrzsCYJNtwaP9m-iazDkSl-wo8vIlOfalGuQVB5G5Z0fvpogzLmTq7ui6Vatg2c6XlBgv3P5aMR2XV0QGTNMrSrgBM6VKQMEqfmZFPJT1mcjBtzrB-X5ERdPb4vy4Yx4WKOZ8i7XAFJyzHDV6v~DFi-1wUT4Nac8ePkmOlR7jNo~4wEvyBPCgg5qBhgHFWRsIx0FUY6T3u44O0tTDa2vGl8rUYRCsHctIAvhfjpdH0wxBgQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"}],"urls":[{"id":40944628,"url":"https://doi.org/10.1016/j.cma.2018.06.034"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239386"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer"><img alt="Research paper thumbnail of Topology optimization of electrode patterns for electroosmotic micromixer" class="work-thumbnail" src="https://attachments.academia-assets.com/113148673/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer">Topology optimization of electrode patterns for electroosmotic micromixer</a></div><div class="wp-workCard_item"><span>International Journal of Heat and Mass Transfer</span><span>, Nov 1, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="cd2e53cccd605f35e3763e0873db4aae" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148673,"asset_id":117239386,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239386"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239386"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239386; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239386]").text(description); $(".js-view-count[data-work-id=117239386]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239386; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239386']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239386, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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The shape and position of electrode pairs, whose induced charges are in contact with the fluid, determine the electric field and hence the resulting fluid-dynamic velocity distribution. In this paper, we address the inverse design of the electrode-pair patterns in such actuation mechanisms. Our approach is to use topology optimization to inversely determine the patterns of an electrode pair. The optimization procedure requires a mathematical description of the desired fluid behaviour, and then drives the patterns of the electrode pairs to achieve the goal performance. We demonstrate the behaviour of the procedure, which couples the Navier-Stokes equations with charge transportation, to implement an efficient electroosmotic micromixer for laminar microflow. We show that the procedure allows to investigate such microflows under the influence of selected parameter variations, thereby exploring the design space towards optimal device performance. This developed method is novel on the topology optimization of a surface structure to control bulk performance and its implementation over a lower-dimensional surface of an otherwise volumetric domain, where the material interpolation is implemented between Dirichlet and Newmann types of boundary conditions.","publication_date":{"day":1,"month":11,"year":2018,"errors":{}},"publication_name":"International Journal of Heat and Mass Transfer","grobid_abstract_attachment_id":113148673},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239386/Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer","translated_internal_url":"","created_at":"2024-04-08T11:24:36.353-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148673,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148673/thumbnails/1.jpg","file_name":"j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7.pdf","download_url":"https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Topology_optimization_of_electrode_patte.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148673/j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7-libre.pdf?1712605018=\u0026response-content-disposition=attachment%3B+filename%3DTopology_optimization_of_electrode_patte.pdf\u0026Expires=1733027840\u0026Signature=KBmZfbHIFtsdmEi8e6AObdiCq4KLiFctRpqigjHc28EOFLRYRuU5nd62R~P-de0VYkP8FpcWNbvlhqhl1wPW-FOfn0l6A~3vEV4ND8QIwD9BtfnMHdIvOIRlnitLR8E4yqfVq7UasigwUhXiguE9vDArt-ZpO1tgu4QmQzE9bIoMlfmWCar1oHzcuSBIBEUzoFwWODrmKRD3OFn0Q3jDBoLE094vpS7cp41R8uQkCK6L9kStdTFTDi-m3Oss3qNe5PUydZFv6zOyWQvuo9BdmoavQ~~9DznGNnjDzG89veCWeJ9IXVIRv4oR29Teb2SzZ0ALpJofSDfHF7kB~jfmuw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Topology_optimization_of_electrode_patterns_for_electroosmotic_micromixer","translated_slug":"","page_count":17,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148673,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148673/thumbnails/1.jpg","file_name":"j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7.pdf","download_url":"https://www.academia.edu/attachments/113148673/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Topology_optimization_of_electrode_patte.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148673/j.ijheatmasstransfer.2018.06.06520240408-1-qxbyf7-libre.pdf?1712605018=\u0026response-content-disposition=attachment%3B+filename%3DTopology_optimization_of_electrode_patte.pdf\u0026Expires=1733027840\u0026Signature=KBmZfbHIFtsdmEi8e6AObdiCq4KLiFctRpqigjHc28EOFLRYRuU5nd62R~P-de0VYkP8FpcWNbvlhqhl1wPW-FOfn0l6A~3vEV4ND8QIwD9BtfnMHdIvOIRlnitLR8E4yqfVq7UasigwUhXiguE9vDArt-ZpO1tgu4QmQzE9bIoMlfmWCar1oHzcuSBIBEUzoFwWODrmKRD3OFn0Q3jDBoLE094vpS7cp41R8uQkCK6L9kStdTFTDi-m3Oss3qNe5PUydZFv6zOyWQvuo9BdmoavQ~~9DznGNnjDzG89veCWeJ9IXVIRv4oR29Teb2SzZ0ALpJofSDfHF7kB~jfmuw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":20097,"name":"Topology Optimization","url":"https://www.academia.edu/Documents/in/Topology_Optimization"},{"id":33661,"name":"Heat and Mass Transfer","url":"https://www.academia.edu/Documents/in/Heat_and_Mass_Transfer"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":909150,"name":"Electrode","url":"https://www.academia.edu/Documents/in/Electrode"}],"urls":[{"id":40944626,"url":"https://doi.org/10.1016/j.ijheatmasstransfer.2018.06.065"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239384"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip"><img alt="Research paper thumbnail of A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip">A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip</a></div><div class="wp-workCard_item"><span>Modern Physics Letters B</span><span>, Apr 16, 2020</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A transient continuum model of the ODEP chip containing single circular particle inside is constr...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239384"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239384"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239384; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239384]").text(description); $(".js-view-count[data-work-id=117239384]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239384; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239384']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239384, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239384]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239384,"title":"A full-scale computational study on the electrodynamics of a rigid particle in an optically induced dielectrophoresis chip","translated_title":"","metadata":{"abstract":"A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.","publisher":"World Scientific","publication_date":{"day":16,"month":4,"year":2020,"errors":{}},"publication_name":"Modern Physics Letters B"},"translated_abstract":"A transient continuum model of the ODEP chip containing single circular particle inside is constructed based on multi-physical field coupling. The dielectrophoresis force and liquid viscous resistance acting on particle are calculated by employing the full Maxwell stress tensor. The coupled flow field, electric field and particle are solved by the arbitrary Lagrange–Euler (ALE) method simultaneously. The throughout dynamic process of particle in the ODEP chip is demonstrated, and the effect of several critical parameters on particle electrodynamics is illuminated. The additional disturbing effect of the photoconductive layer on the electric field as well as the micro-channel wall on the flow field is presented to clarify the particle motion in the vertical direction. The results in this study provide a detailed understanding of the particle dynamics in the ODEP chip.","internal_url":"https://www.academia.edu/117239384/A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip","translated_internal_url":"","created_at":"2024-04-08T11:24:36.135-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"A_full_scale_computational_study_on_the_electrodynamics_of_a_rigid_particle_in_an_optically_induced_dielectrophoresis_chip","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":27372,"name":"Dielectrophoresis","url":"https://www.academia.edu/Documents/in/Dielectrophoresis"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field"},{"id":2807557,"name":"Maxwell stress tensor","url":"https://www.academia.edu/Documents/in/Maxwell_stress_tensor"}],"urls":[{"id":40944625,"url":"https://doi.org/10.1142/s0217984920502334"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239383"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis"><img alt="Research paper thumbnail of Continuous separation of microparticles based on optically induced dielectrophoresis" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis">Continuous separation of microparticles based on optically induced dielectrophoresis</a></div><div class="wp-workCard_item"><span>Microfluidics and Nanofluidics</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">To achieve high-throughput and high-efficiency separation based on optically induced dielectropho...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239383"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239383"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239383; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239383]").text(description); $(".js-view-count[data-work-id=117239383]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239383; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239383']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239383, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=117239383]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239383,"title":"Continuous separation of microparticles based on optically induced dielectrophoresis","translated_title":"","metadata":{"abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","publisher":"Springer Science+Business Media","publication_date":{"day":null,"month":null,"year":2022,"errors":{}},"publication_name":"Microfluidics and Nanofluidics"},"translated_abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","internal_url":"https://www.academia.edu/117239383/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_internal_url":"","created_at":"2024-04-08T11:24:35.923-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":27372,"name":"Dielectrophoresis","url":"https://www.academia.edu/Documents/in/Dielectrophoresis"},{"id":317912,"name":"Microfluidics and Nanofluidics","url":"https://www.academia.edu/Documents/in/Microfluidics_and_Nanofluidics"},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering"},{"id":1130559,"name":"Electric Field","url":"https://www.academia.edu/Documents/in/Electric_Field"},{"id":3849972,"name":"Springer Nature","url":"https://www.academia.edu/Documents/in/Springer_Nature"}],"urls":[{"id":40944623,"url":"https://doi.org/10.1007/s10404-021-02512-0"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239381"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239381/Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel"><img alt="Research paper thumbnail of Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel" class="work-thumbnail" src="https://attachments.academia-assets.com/113148674/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239381/Dielectrophoretic_choking_phenomenon_of_a_deformable_particle_in_a_converging_diverging_microchannel">Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel</a></div><div class="wp-workCard_item"><span>Electrophoresis</span><span>, Dec 27, 2017</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="01198ce7dc34be42b483cf22bd8e0fd7" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148674,"asset_id":117239381,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148674/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239381"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239381"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239381; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239381]").text(description); $(".js-view-count[data-work-id=117239381]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239381; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239381']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239381, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "01198ce7dc34be42b483cf22bd8e0fd7" } } $('.js-work-strip[data-work-id=117239381]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239381,"title":"Dielectrophoretic choking phenomenon of a deformable particle in a converging-diverging microchannel","translated_title":"","metadata":{"publisher":"Wiley","grobid_abstract":"The translational motion of small particles in an electrokinetic fluid flow through a constriction can be enhanced by an increase of the applied electric potential. Beyond a critical potential, however, the negative dielectrophoresis (DEP) can overpower other forces to prevent particles that are even smaller than the constriction from passing through the constriction. This DEP choking phenomenon was studied previously for rigid particles. Here, the DEP choking phenomenon is revisited for deformable particles, which are ubiquitous in many biomedical applications. Particle deformability is measured by the particle shear modulus, and the choking conditions are reported through a parametric study that includes the channel geometry, external electric potential, and particle zeta potential. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239379"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure"><img alt="Research paper thumbnail of An Enhanced Electroosmotic Micromixer with an Efficient Asymmetric Lateral Structure" class="work-thumbnail" src="https://attachments.academia-assets.com/113148620/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure">An Enhanced Electroosmotic Micromixer with an Efficient Asymmetric Lateral Structure</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, Dec 1, 2016</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0c7ea617a5008de962a43db946c08ac1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148620,"asset_id":117239379,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239379"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239379"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239379; 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Here, an efficient electroosmotic micromixer based on a carefully designed lateral structure is demonstrated. The electroosmotic flow in this mixer with an asymmetrical structure induces enhanced disturbance in the micro channel, helping the fluid streams' folding and stretching, thereby enabling appreciable mixing. Quantitative analysis of the mixing efficiency with respect to the potential applied and the flow rate suggests that the electroosmotic microfluidic mixer developed in the present work can achieve efficient mixing with low applied potential.","publication_date":{"day":1,"month":12,"year":2016,"errors":{}},"publication_name":"Micromachines","grobid_abstract_attachment_id":113148620},"translated_abstract":null,"internal_url":"https://www.academia.edu/117239379/An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure","translated_internal_url":"","created_at":"2024-04-08T11:24:35.565-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148620,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148620/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"An_Enhanced_Electroosmotic_Micromixer_wi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148620/pdf-libre.pdf?1712605022=\u0026response-content-disposition=attachment%3B+filename%3DAn_Enhanced_Electroosmotic_Micromixer_wi.pdf\u0026Expires=1733027840\u0026Signature=b0Ea38tKg~ekB94Gn5zgJ-hgbHzw1dO1vmJNGCCA9R1rF5ohcciVlFguRwGJ3ZIzxTdW~UhHB5p8h--jn2CGvUWbdSDRwytgDmX28VsEyQdPAa6AHiicjC9s2fuXmN2RuiGQlKZnjW0WqWSNaSDQb30jkG7D3euyEVbrZoyKa8uxaevfUNt6A2uia7~GBl6H4x5LYgBMw6DBMehPBqd8RnBOEdTGqQ4sOsbsljKLdaR55VZbo8C93N0VJ1F5uOwXomBONTsyY-LFySC417T4UFq-9re-PnBN7J1Z1p-CsBODlKhs0TsyqaUJlUwzcKIoTZhtQU53cssI-MndU~DBnA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"An_Enhanced_Electroosmotic_Micromixer_with_an_Efficient_Asymmetric_Lateral_Structure","translated_slug":"","page_count":8,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148620,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148620/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/113148620/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"An_Enhanced_Electroosmotic_Micromixer_wi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148620/pdf-libre.pdf?1712605022=\u0026response-content-disposition=attachment%3B+filename%3DAn_Enhanced_Electroosmotic_Micromixer_wi.pdf\u0026Expires=1733027840\u0026Signature=b0Ea38tKg~ekB94Gn5zgJ-hgbHzw1dO1vmJNGCCA9R1rF5ohcciVlFguRwGJ3ZIzxTdW~UhHB5p8h--jn2CGvUWbdSDRwytgDmX28VsEyQdPAa6AHiicjC9s2fuXmN2RuiGQlKZnjW0WqWSNaSDQb30jkG7D3euyEVbrZoyKa8uxaevfUNt6A2uia7~GBl6H4x5LYgBMw6DBMehPBqd8RnBOEdTGqQ4sOsbsljKLdaR55VZbo8C93N0VJ1F5uOwXomBONTsyY-LFySC417T4UFq-9re-PnBN7J1Z1p-CsBODlKhs0TsyqaUJlUwzcKIoTZhtQU53cssI-MndU~DBnA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":225478,"name":"Electro-Osmosis","url":"https://www.academia.edu/Documents/in/Electro-Osmosis"},{"id":895043,"name":"Micromixer","url":"https://www.academia.edu/Documents/in/Micromixer"},{"id":1008960,"name":"Reynolds Number","url":"https://www.academia.edu/Documents/in/Reynolds_Number"}],"urls":[{"id":40944621,"url":"https://www.mdpi.com/2072-666X/7/12/218/pdf?version=1480598050"}]}, dispatcherData: dispatcherData }); 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239374"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip"><img alt="Research paper thumbnail of Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip" class="work-thumbnail" src="https://attachments.academia-assets.com/113148664/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip">Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip</a></div><div class="wp-workCard_item"><span>Frontiers in Chemistry</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testi...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1f0f6d37c7c4af84cd1520282c6aa2a4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148664,"asset_id":117239374,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239374"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239374"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239374; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239374]").text(description); $(".js-view-count[data-work-id=117239374]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239374; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239374']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239374, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "1f0f6d37c7c4af84cd1520282c6aa2a4" } } $('.js-work-strip[data-work-id=117239374]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239374,"title":"Point-of-Care Testing for Multiple Cardiac Markers Based on a Snail-Shaped Microfluidic Chip","translated_title":"","metadata":{"abstract":"Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.","publisher":"Frontiers Media SA","ai_title_tag":"Multiplex Cardiac Marker Detection with Snail-Shaped Chip","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Frontiers in Chemistry"},"translated_abstract":"Existing methods for detecting cardiac markers are difficult to be applied in point-of-care testing (POCT) due to complex operation, long time consumption, and low sensitivity. Here, we report a snail-shaped microfluidic chip (SMC) for the multiplex detection of cTnI, CK-MB, and Myo with high sensitivity and a short detection time. The SMC consists of a sandwich structure: a channel layer with a mixer and reaction zone, a reaction layer coated with capture antibodies, and a base layer. The opening or closing of the microchannels is realized by controlling the downward movement of the press-type mechanical valve. The chemiluminescence method was used as a signal readout, and the experimental conditions were optimized. SMC could detect cTnI, CK-MB, and Myo at concentrations as low as 1.02, 1.37, and 4.15. The SMC will be a promising platform for a simultaneous determination of multianalytes and shows a potential application in POCT.","internal_url":"https://www.academia.edu/117239374/Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip","translated_internal_url":"","created_at":"2024-04-08T11:24:34.821-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":113148664,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148664/thumbnails/1.jpg","file_name":"fchem-09-741058.pdf","download_url":"https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Point_of_Care_Testing_for_Multiple_Cardi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148664/fchem-09-741058-libre.pdf?1712605017=\u0026response-content-disposition=attachment%3B+filename%3DPoint_of_Care_Testing_for_Multiple_Cardi.pdf\u0026Expires=1733027840\u0026Signature=dGqw9fFDg598JhPwrIf9N3D~fXQhpNsQ066~1YiBehpNWfIZWBSxoIPxOvECDDAzaitKW5T19OrP0JsGdbR6dzqj32hrG8T7ormLLfRNYAUwbOxCwz9XzDu51UYGmqG8XFiG5r1~4F-u9p~dM3Q-yHNQ09Gbvgx8wv9cuLK6zgUedoWYclNbPIIrNRgXokDuXFy~QSb0nxMCIyms8Qq0gP~F0dQoQm~0UENqaX-5oPTeqsF2YtT0GiTAXIWWZHmXbGVmow2f~HinaTpGn4Uc8Ya6z424reO1YxU8krcq-5qGzTA2NRR9RWuwS7Tn0Nq1aGdJlIO7oLlQ7aVgaxDwvQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Point_of_Care_Testing_for_Multiple_Cardiac_Markers_Based_on_a_Snail_Shaped_Microfluidic_Chip","translated_slug":"","page_count":11,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":113148664,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/113148664/thumbnails/1.jpg","file_name":"fchem-09-741058.pdf","download_url":"https://www.academia.edu/attachments/113148664/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Point_of_Care_Testing_for_Multiple_Cardi.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/113148664/fchem-09-741058-libre.pdf?1712605017=\u0026response-content-disposition=attachment%3B+filename%3DPoint_of_Care_Testing_for_Multiple_Cardi.pdf\u0026Expires=1733027840\u0026Signature=dGqw9fFDg598JhPwrIf9N3D~fXQhpNsQ066~1YiBehpNWfIZWBSxoIPxOvECDDAzaitKW5T19OrP0JsGdbR6dzqj32hrG8T7ormLLfRNYAUwbOxCwz9XzDu51UYGmqG8XFiG5r1~4F-u9p~dM3Q-yHNQ09Gbvgx8wv9cuLK6zgUedoWYclNbPIIrNRgXokDuXFy~QSb0nxMCIyms8Qq0gP~F0dQoQm~0UENqaX-5oPTeqsF2YtT0GiTAXIWWZHmXbGVmow2f~HinaTpGn4Uc8Ya6z424reO1YxU8krcq-5qGzTA2NRR9RWuwS7Tn0Nq1aGdJlIO7oLlQ7aVgaxDwvQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"},{"id":914941,"name":"Point of Care Testing","url":"https://www.academia.edu/Documents/in/Point_of_Care_Testing"}],"urls":[{"id":40944616,"url":"https://www.frontiersin.org/articles/10.3389/fchem.2021.741058/full"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="117239373"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/117239373/Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion"><img alt="Research paper thumbnail of Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion" class="work-thumbnail" src="https://attachments.academia-assets.com/113148617/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/117239373/Robust_sulfonated_poly_ether_ether_ketone_nanochannels_for_high_performance_osmotic_energy_conversion">Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion</a></div><div class="wp-workCard_item"><span>National Science Review</span><span>, 2020</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting c...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting clean and sustainable osmotic energy existing in the salinity gradient. However, the current designs of membranes cannot cope with the high output power density and robustness. Here, we construct a sulfonated poly (ether ether ketone) (SPEEK) nanochannel membrane with numerous nanochannels for a membrane-based osmotic power generator. The parallel nanochannels with high space charges show excellent cation-selectivity, which could further be improved by adjusting the length and charge density of nanochannels. Based on numerical simulation, the system with space charge shows better conductivity and selectivity than those of a surface-charged nanochannel. The output power density of our proposed membrane-based device reaches up to 5.8 W/m2 by mixing artificial seawater and river water. Additionally, the SPEEK membranes exhibit good mechanical properties, endowing the possibility of creating ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ffd518629692aa93c622c80c223c51f5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":113148617,"asset_id":117239373,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/113148617/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="117239373"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="117239373"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 117239373; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=117239373]").text(description); $(".js-view-count[data-work-id=117239373]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 117239373; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='117239373']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 117239373, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "ffd518629692aa93c622c80c223c51f5" } } $('.js-work-strip[data-work-id=117239373]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":117239373,"title":"Robust sulfonated poly (ether ether ketone) nanochannels for high-performance osmotic energy conversion","translated_title":"","metadata":{"abstract":"The membrane-based reverse electrodialysis (RED) technique has a fundamental role in harvesting clean and sustainable osmotic energy existing in the salinity gradient. 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The layout of channel networks can be rather simple, with constant width, straight channels, or the layout can be very complex, with multiple splitters, combiners, or even multiple layers. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="100626520"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/100626520/Combustion_Characteristics_of_Small_Laminar_Flames_in_an_Upward_Decreasing_Magnetic_Field"><img alt="Research paper thumbnail of Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field" class="work-thumbnail" src="https://attachments.academia-assets.com/101395892/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626520/Combustion_Characteristics_of_Small_Laminar_Flames_in_an_Upward_Decreasing_Magnetic_Field">Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field</a></div><div class="wp-workCard_item"><span>Energies</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1a468d1fbd581995a410a0edc333e9a8" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395892,"asset_id":100626520,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395892/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626520"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626520"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626520; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=100626520]").text(description); $(".js-view-count[data-work-id=100626520]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 100626520; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='100626520']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 100626520, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "1a468d1fbd581995a410a0edc333e9a8" } } $('.js-work-strip[data-work-id=100626520]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":100626520,"title":"Combustion Characteristics of Small Laminar Flames in an Upward Decreasing Magnetic Field","translated_title":"","metadata":{"abstract":"The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of ...","publisher":"MDPI AG","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Energies"},"translated_abstract":"The combustion characteristics of laminar biogas premixed and diffusion flames in the presence of upward decreasing magnetic fields have been investigated in this study. The mechanism of magnet–flame interaction in the literature, in which magnetic fields change the behaviors of laminar flames due to the paramagnetic and diamagnetic properties of the constituent gases, is examined and the results are as follows. The magnetic field has no noticeable effect on premixed flames due to low oxygen concentration of the mixed gas at the injection and the relatively high flow momentum. However, due to the diffusion nature of diffusion flames and paramagnetic property of oxygen in ambient air, oxygen distributions are subjected to the gradient of magnetic flux, thus shortening the height of diffusion flames. Results also show that the flame volume is more strongly varied than flame height. Altered oxygen distributions result in improved combustion and higher flame temperature. In the case of 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Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":6263,"name":"Combustion","url":"https://www.academia.edu/Documents/in/Combustion"},{"id":34754,"name":"Magnetic field","url":"https://www.academia.edu/Documents/in/Magnetic_field"},{"id":83315,"name":"Diffusion","url":"https://www.academia.edu/Documents/in/Diffusion"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":176527,"name":"Laminar Flow","url":"https://www.academia.edu/Documents/in/Laminar_Flow"},{"id":511019,"name":"Diamagnetism","url":"https://www.academia.edu/Documents/in/Diamagnetism"},{"id":832176,"name":"Diffusion Flame","url":"https://www.academia.edu/Documents/in/Diffusion_Flame"},{"id":1011047,"name":"Laminar Flame Speed","url":"https://www.academia.edu/Documents/in/Laminar_Flame_Speed"},{"id":1290065,"name":"ENERGIES","url":"https://www.academia.edu/Documents/in/ENERGIES-1"},{"id":2980369,"name":"Paramagnetism","url":"https://www.academia.edu/Documents/in/Paramagnetism"}],"urls":[{"id":30849375,"url":"https://www.mdpi.com/1996-1073/14/7/1969/pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="100626519"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/100626519/Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions"><img alt="Research paper thumbnail of Enzyme Method-Based Microfluidic Chip for the Rapid Detection of Copper Ions" class="work-thumbnail" src="https://attachments.academia-assets.com/101395891/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626519/Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions">Enzyme Method-Based Microfluidic Chip for the Rapid Detection of Copper Ions</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Metal ions in high concentrations can pollute the marine environment. Human activities and indust...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5e20507e3a59f59594fd639605e9f2a4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395891,"asset_id":100626519,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626519; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=100626519]").text(description); $(".js-view-count[data-work-id=100626519]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 100626519; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='100626519']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 100626519, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "5e20507e3a59f59594fd639605e9f2a4" } } $('.js-work-strip[data-work-id=100626519]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":100626519,"title":"Enzyme Method-Based Microfluidic Chip for the Rapid Detection of Copper Ions","translated_title":"","metadata":{"abstract":"Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...","publisher":"MDPI AG","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Micromachines"},"translated_abstract":"Metal ions in high concentrations can pollute the marine environment. Human activities and industrial pollution are the causes of Cu2+ contamination. Here, we report our discovery of an enzyme method-based microfluidic that can be used to rapidly detect Cu2+ in seawater. In this method, Cu2+ is reduced to Cu+ to inhibit horseradish peroxidase (HRP) activity, which then results in the color distortion of the reaction solution. The chip provides both naked eye and spectrophotometer modalities. Cu2+ concentrations have an ideal linear relationship, with absorbance values ranging from 3.91 nM to 256 μM. The proposed enzyme method-based microfluidic chip detects Cu2+ with a limit of detection (LOD) of 0.87 nM. Other common metal ions do not affect the operation of the chip. The successful detection of Cu2+ was achieved using three real seawater samples, verifying the ability of the chip in practical applications. Furthermore, the chip realizes the functions of two AND gates in series and...","internal_url":"https://www.academia.edu/100626519/Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions","translated_internal_url":"","created_at":"2023-04-23T07:09:30.901-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":101395891,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395891/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395891/pdf-libre.pdf?1682280149=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Cv08s3KkiwZ9mDDK50nH5xYaa6UDaPQ5oaT4WTuNhdfRURGADkx8Uw87keqp45S-V1I0czFJwkj0JzZYq7uPDG4fBenLYlS4GOvati4u-VQJnPGkzRFOLdjp9JA6s8Ei9ffm~2pTog6fw1a~I9E96ELFUVpwLkCO2Ztj5~1wYZ2rdMnDTZJ7tN5QSO5RGl1bTOwxS8fX9sRcI6uR9CLXvxry0tBYxOvyM1-4Ahg5cvAftyU1lf4eGt4f4l~dKknm09M5Vo3nEDu4MXTjSYwsj9fNJDXegfKygPecGJG3iw3f8GDyqd83M4wFKfpJ8vpKT4Mtq8daWtCj~8GYLllRCQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Enzyme_Method_Based_Microfluidic_Chip_for_the_Rapid_Detection_of_Copper_Ions","translated_slug":"","page_count":10,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":101395891,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395891/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395891/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395891/pdf-libre.pdf?1682280149=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Cv08s3KkiwZ9mDDK50nH5xYaa6UDaPQ5oaT4WTuNhdfRURGADkx8Uw87keqp45S-V1I0czFJwkj0JzZYq7uPDG4fBenLYlS4GOvati4u-VQJnPGkzRFOLdjp9JA6s8Ei9ffm~2pTog6fw1a~I9E96ELFUVpwLkCO2Ztj5~1wYZ2rdMnDTZJ7tN5QSO5RGl1bTOwxS8fX9sRcI6uR9CLXvxry0tBYxOvyM1-4Ahg5cvAftyU1lf4eGt4f4l~dKknm09M5Vo3nEDu4MXTjSYwsj9fNJDXegfKygPecGJG3iw3f8GDyqd83M4wFKfpJ8vpKT4Mtq8daWtCj~8GYLllRCQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":101395890,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395890/thumbnails/1.jpg","file_name":"pdf.pdf","download_url":"https://www.academia.edu/attachments/101395890/download_file","bulk_download_file_name":"Enzyme_Method_Based_Microfluidic_Chip_fo.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395890/pdf-libre.pdf?1682280152=\u0026response-content-disposition=attachment%3B+filename%3DEnzyme_Method_Based_Microfluidic_Chip_fo.pdf\u0026Expires=1733027841\u0026Signature=Zz93gQY02LnYKwmM10RseTcM~SYe-CQaDUfdibIBuRYMXm-rU2599s1kjhF3bB~ktfwWTZhwTXiwNWawJdmr2ZT5rQkDgQmYz2zN0SM7yOxVv~v26rB4pQ23qISgNHPbarDNQbqGaTcFG4fLpxSjBUjVH0MgLvDa0-Kh~oYZD2P93qARmmwmRPUbctvsn~gGjKYL8lfPU~OViWTN1--SxDMlb3UVC4e-Kuqnitc0ba0inVoUe1CxoMNB-4vbclprpcgaogFbeuoRDesyHphPjyKhuMzKSAc4Za4~-6Mxr8Gx30bgSQX2wW-OOwvfMFB-9u0jf9c~k1WEy6VS-suIIQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":2721,"name":"Microfluidics","url":"https://www.academia.edu/Documents/in/Microfluidics"},{"id":80692,"name":"Copper","url":"https://www.academia.edu/Documents/in/Copper"},{"id":184467,"name":"Seawater","url":"https://www.academia.edu/Documents/in/Seawater"},{"id":322954,"name":"Chip","url":"https://www.academia.edu/Documents/in/Chip"},{"id":753116,"name":"Absorbance","url":"https://www.academia.edu/Documents/in/Absorbance"},{"id":2465388,"name":"Naked Eye","url":"https://www.academia.edu/Documents/in/Naked_Eye"}],"urls":[{"id":30849374,"url":"https://www.mdpi.com/2072-666X/12/11/1380/pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="100626518"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity"><img alt="Research paper thumbnail of Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity" class="work-thumbnail" src="https://attachments.academia-assets.com/101395918/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity">Inversely designed micro-textures for robust Cassie–Baxter mode of super-hydrophobicity</a></div><div class="wp-workCard_item"><span>Computer Methods in Applied Mechanics and Engineering</span><span>, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b52599d72a820fafff221a89b61abb82" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":101395918,"asset_id":100626518,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="100626518"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="100626518"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 100626518; 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To meet this purpose, we propose an inverse computational design procedure for the discovery of suitable periodic micro-textures, based on three different tilings of the plane. The symmetric tiles of the lattice are regular triangles, quadrangles, and hexagons. The goal of the inverse design procedure is to achieve the robust Cassie-Baxter state, in which the liquid/vapour interface is mathematically described using the Young-Laplace equation on the lattice, and a topology optimisation approach is utilised to construct a variational problem for the inverse design procedure. Based on numerical calculations of the constructed variational problem, underlying effects are revealed for several factors, including the Bond number, duty ratio, feature size, and lattice constant. The effects of feature size and lattice constant provide approaches for compromisingly considering the robustness of the Cassie-Baxter mode and manufacturability of the inversely designed micro-textures; the effect of the lattice constant permits the scaling properties of the derived patterns, and this in turn provides an approach to avoid the elasto-capillary instability driven collapse of the micro/nanostructures in the derived micro-textures. Further, a monolithic inverse design procedure for the periodic micro-textures is proposed in the conclusions, with synthetically considering the manufacturability as well as contact angle and surface-volume ratio of the liquid bulge held by the supported liquid/vapour interface.","publication_date":{"day":null,"month":null,"year":2018,"errors":{}},"publication_name":"Computer Methods in Applied Mechanics and Engineering","grobid_abstract_attachment_id":101395918},"translated_abstract":null,"internal_url":"https://www.academia.edu/100626518/Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_internal_url":"","created_at":"2023-04-23T07:09:30.731-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":101395918,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395918/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420230423-1-ia3as3.pdf","download_url":"https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395918/j.cma.2018.06.03420230423-1-ia3as3-libre.pdf?1682280490=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027841\u0026Signature=a4JCfXHOeIjDCrkeJ0FCYs9bbNnGl4Zq168b0PNuHlVhYhfyFpbZbJRACpSmOKj-ZM3ARnH5CByWQpsRRINy0IpHQkLERcNMTnna0Er3jlG3nt3kvZYMxEK22lwLJ4x8Bs3~WcmbnPFD9CztsPEAdN2BJT~VytvD6R78Ds0aZy2WDLh4-ClvvXGgBSn8OIGLS~ZDBx1J-fUe-fhZFAu4OXDJuuJx6K8OSSuzoy3oZ1b4qMKKt9veE8MOHsDE61ghd4gDr3A0P2Y60wsL0otupnX6msbMImpRdPgcQlzwbFNGt9ZXywT7Ix0ZVcT5tG9R0ouD9mpzt83qeGraGu8Vig__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Inversely_designed_micro_textures_for_robust_Cassie_Baxter_mode_of_super_hydrophobicity","translated_slug":"","page_count":23,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":101395918,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/101395918/thumbnails/1.jpg","file_name":"j.cma.2018.06.03420230423-1-ia3as3.pdf","download_url":"https://www.academia.edu/attachments/101395918/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Inversely_designed_micro_textures_for_ro.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/101395918/j.cma.2018.06.03420230423-1-ia3as3-libre.pdf?1682280490=\u0026response-content-disposition=attachment%3B+filename%3DInversely_designed_micro_textures_for_ro.pdf\u0026Expires=1733027841\u0026Signature=a4JCfXHOeIjDCrkeJ0FCYs9bbNnGl4Zq168b0PNuHlVhYhfyFpbZbJRACpSmOKj-ZM3ARnH5CByWQpsRRINy0IpHQkLERcNMTnna0Er3jlG3nt3kvZYMxEK22lwLJ4x8Bs3~WcmbnPFD9CztsPEAdN2BJT~VytvD6R78Ds0aZy2WDLh4-ClvvXGgBSn8OIGLS~ZDBx1J-fUe-fhZFAu4OXDJuuJx6K8OSSuzoy3oZ1b4qMKKt9veE8MOHsDE61ghd4gDr3A0P2Y60wsL0otupnX6msbMImpRdPgcQlzwbFNGt9ZXywT7Ix0ZVcT5tG9R0ouD9mpzt83qeGraGu8Vig__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering"},{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"}],"urls":[{"id":30849373,"url":"https://api.elsevier.com/content/article/PII:S0045782518303323?httpAccept=text/xml"}]}, dispatcherData: dispatcherData }); 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Although both potential and pH gradient can significantly change the performance of ion current rectification in nanoscale, the potential mechanism is still not fully understood. In this study, the ion current rectification, surface charge distribution and ion selectivity of silica nanopore under different background salt concentration and pH gradient were discussed by an analytical model, which takes into account the effects of electroosmotic flow, multiple ionic species, and the acid base neutralization. The results show that the polarity of nanopore rectifier can be changed by changing the acidity and alkalinity at both ends of the nanopore. For the first time, we find that the rectification polarity of silica conical nanopore exhibits different performances under high and low electric field intensity. One case in this study shows the rectification ratio curve of the nanopore will have a maximum or minimum value and the extreme point is near the zero of the ion current. With the increase of the concentration of background salt solution, the voltage at the zero point of ion current approaches the zero point, and then the maximum or minimum point moves to the left. The extreme point offset and polarity reversal phenomena may have potential application value in nanopore-based sensing devices.","publication_date":{"day":null,"month":null,"year":2020,"errors":{}},"publication_name":"SN Applied Sciences","grobid_abstract_attachment_id":84351649},"translated_abstract":null,"internal_url":"https://www.academia.edu/76752476/The_polarization_reverse_of_diode_like_conical_nanopore_under_pH_gradient","translated_internal_url":"","created_at":"2022-04-17T16:37:23.635-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":84351649,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351649/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351649/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351649/s42452-020-03675-1-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=TrQBeIN5o2P57Womyo~Rrz5Ct60SsyMuVIq8D5ythld69jyvEdBMJ8USPDtF8KjKZL30FWLzXa9E~r9WpURol0ANNGgfvzhTlh9ILH1bxRtTLux1WDFXe7KEe4YalTnV3~m90h8chgBc6mZdJumbP1Ro3Ug-LpNQLCEOF7xPZaX3aiSRdwJisWJfLUH~zg5L4edElEdOm1nUAnexuji46n2AWcAwhmZvBap4FkkdLt8Y~y2QLYX0dIGrDRtTW~PP7rSEy1WiqmzDObvug20KnCfu6jVZAILWQmddIJVDsYWkPgVleS5euWx9YzKfJ-QAISmksa7hltmqzp~cF4LSrA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"The_polarization_reverse_of_diode_like_conical_nanopore_under_pH_gradient","translated_slug":"","page_count":14,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":84351649,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351649/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351649/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351649/s42452-020-03675-1-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=TrQBeIN5o2P57Womyo~Rrz5Ct60SsyMuVIq8D5ythld69jyvEdBMJ8USPDtF8KjKZL30FWLzXa9E~r9WpURol0ANNGgfvzhTlh9ILH1bxRtTLux1WDFXe7KEe4YalTnV3~m90h8chgBc6mZdJumbP1Ro3Ug-LpNQLCEOF7xPZaX3aiSRdwJisWJfLUH~zg5L4edElEdOm1nUAnexuji46n2AWcAwhmZvBap4FkkdLt8Y~y2QLYX0dIGrDRtTW~PP7rSEy1WiqmzDObvug20KnCfu6jVZAILWQmddIJVDsYWkPgVleS5euWx9YzKfJ-QAISmksa7hltmqzp~cF4LSrA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":84351650,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351650/thumbnails/1.jpg","file_name":"s42452-020-03675-1.pdf","download_url":"https://www.academia.edu/attachments/84351650/download_file","bulk_download_file_name":"The_polarization_reverse_of_diode_like_c.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351650/s42452-020-03675-1-libre.pdf?1650239167=\u0026response-content-disposition=attachment%3B+filename%3DThe_polarization_reverse_of_diode_like_c.pdf\u0026Expires=1733027841\u0026Signature=MFSQp2pyl81D6S1771KrZ~50WhSSF9qir44t3XHsOl0iFMVarvT0nyLKBDZyyjEHl~GxCRmOApF1Rvl4lW5pKg-ShzoiKojCLaoWW0p-7ir-WEv4g6aoQ~zswRbq7RVZVs6PDmvL-R9ach~1lX2Smmc3eCsS2iy-QMBcgfJmAy4z1vGLz1YhF6yMS1~aUCgDrJ0cNM4dqC4hX~~Kty4oWEW0~MGtTUDCpFOKUW6Jft4KA2hK70UpFj918TNy1dK0xjb9tnh~m2DKsUj4ic7lU~wKSBPYlKylvVUYzM0PTaWYivjXibz-w4aNHmIRWcRP1HomkHqiVzSuDxiUnlcozQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":511,"name":"Materials Science","url":"https://www.academia.edu/Documents/in/Materials_Science"}],"urls":[{"id":19595376,"url":"http://link.springer.com/content/pdf/10.1007/s42452-020-03675-1.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="76752475"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis"><img alt="Research paper thumbnail of Continuous separation of microparticles based on optically induced dielectrophoresis" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis">Continuous separation of microparticles based on optically induced dielectrophoresis</a></div><div class="wp-workCard_item"><span>Microfluidics and Nanofluidics</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">To achieve high-throughput and high-efficiency separation based on optically induced dielectropho...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="76752475"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="76752475"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76752475; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76752475]").text(description); $(".js-view-count[data-work-id=76752475]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76752475; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76752475']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76752475, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=76752475]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76752475,"title":"Continuous separation of microparticles based on optically induced dielectrophoresis","translated_title":"","metadata":{"abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","publisher":"Springer Science and Business Media LLC","publication_date":{"day":null,"month":null,"year":2022,"errors":{}},"publication_name":"Microfluidics and Nanofluidics"},"translated_abstract":"To achieve high-throughput and high-efficiency separation based on optically induced dielectrophoresis (ODEP), an ODEP-based transient numerical model containing microparticles is developed under alternating current (AC) electric field coupling with an open flow field. In this model, the MST method is employed to calculate the time-averaged AC DEP force and the fluid viscous resistance acting on the particle, the Arbitrary Lagrangian–Eulerian (ALE) method is used to numerically solve the strong coupling electric-fluid–solid mechanics, and the efficient and continuous separation of microparticles is achieved. The results show that the trajectories of particles with different conductivity are clearly differentiated due to two different DEP actions, which enables separation of particles, and its separation performance can be optimized by adjusting the key parameters, including bright area width, applied alternating current (AC) electric voltage and inlet flow velocity. This study explains the continuous separation mechanism of particles under the combined action of AC electric field and flow field, and provides theoretical support for the design of high-efficiency ODEP microparticles separation device.","internal_url":"https://www.academia.edu/76752475/Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_internal_url":"","created_at":"2022-04-17T16:37:23.492-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Continuous_separation_of_microparticles_based_on_optically_induced_dielectrophoresis","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[],"research_interests":[{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology"},{"id":317912,"name":"Microfluidics and Nanofluidics","url":"https://www.academia.edu/Documents/in/Microfluidics_and_Nanofluidics"},{"id":554780,"name":"Interdisciplinary Engineering","url":"https://www.academia.edu/Documents/in/Interdisciplinary_Engineering"},{"id":3849972,"name":"Springer Nature","url":"https://www.academia.edu/Documents/in/Springer_Nature"}],"urls":[{"id":19595375,"url":"https://link.springer.com/content/pdf/10.1007/s10404-021-02512-0.pdf"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="76752474"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/76752474/Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis"><img alt="Research paper thumbnail of Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis" class="work-thumbnail" src="https://attachments.academia-assets.com/84351648/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/76752474/Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis">Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis</a></div><div class="wp-workCard_item"><span>Micromachines</span><span>, 2021</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on li...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. The current micromixer provides a favorable fluid-mixing method based on an optical virtual electrode, and could promote...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="7eead9f4feabe0fbf281e9fb7cce84ba" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84351648,"asset_id":76752474,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84351648/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="76752474"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="76752474"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76752474; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76752474]").text(description); $(".js-view-count[data-work-id=76752474]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76752474; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76752474']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76752474, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "7eead9f4feabe0fbf281e9fb7cce84ba" } } $('.js-work-strip[data-work-id=76752474]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76752474,"title":"Mixing Mechanism of Microfluidic Mixer with Staggered Virtual Electrode Based on Light-Actuated AC Electroosmosis","translated_title":"","metadata":{"abstract":"In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. The current micromixer provides a favorable fluid-mixing method based on an optical virtual electrode, and could promote...","publisher":"Micromachines","publication_date":{"day":null,"month":null,"year":2021,"errors":{}},"publication_name":"Micromachines"},"translated_abstract":"In this paper, we present a novel microfluidic mixer with staggered virtual electrode based on light-actuated AC electroosmosis (LACE). We solve the coupled system of the flow field described by Navier–Stokes equations, the described electric field by a Laplace equation, and the concentration field described by a convection–diffusion equation via a finite-element method (FEM). Moreover, we study the distribution of the flow, electric, and concentration fields in the microchannel, and reveal the generating mechanism of the rotating vortex on the cross-section of the microchannel and the mixing mechanism of the fluid sample. We also explore the influence of several key geometric parameters such as the length, width, and spacing of the virtual electrode, and the height of the microchannel on mixing performance; the relatively optimal mixer structure is thus obtained. The current micromixer provides a favorable fluid-mixing method based on an optical virtual electrode, and could promote...","internal_url":"https://www.academia.edu/76752474/Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis","translated_internal_url":"","created_at":"2022-04-17T16:37:23.358-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":42451119,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":84351648,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351648/thumbnails/1.jpg","file_name":"micromachines-12-00744-v2.pdf","download_url":"https://www.academia.edu/attachments/84351648/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Mixing_Mechanism_of_Microfluidic_Mixer_w.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351648/micromachines-12-00744-v2-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DMixing_Mechanism_of_Microfluidic_Mixer_w.pdf\u0026Expires=1733027841\u0026Signature=LEAQlYa0~muufOOJ5JeM6UAlLezmuf19tiYXIh4yc0sSYh2L52U2JjsWxnu5z3xtErMdpIi7YJWHGaBdDwqExz0m5KPS3MxgUUlJ1k8GMuxxpdINMEMM1x5iIvXAjLETlI15w4dLNvFQ8Xr44FBfD~Ao3ph83nAV8JYPdi81T87Q4zFS6sm9ohXx0com~VEz~8snlbOgg8aZfHIkgD8QoUMjEZVY4oDxsDvbUrsqLfUddRZhNvMsKqEhSEo8bam2cRNPninfHnDumPO8z9Dv2qdSODIB4KJLZJVC5anoYCbb1xfjsgxWpHXP-NU3C763YOZQfeCCux5LQp6GMZ58zw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Mixing_Mechanism_of_Microfluidic_Mixer_with_Staggered_Virtual_Electrode_Based_on_Light_Actuated_AC_Electroosmosis","translated_slug":"","page_count":14,"language":"en","content_type":"Work","owner":{"id":42451119,"first_name":"Teng","middle_initials":null,"last_name":"Zhou","page_name":"TengZhou","domain_name":"pledco","created_at":"2016-01-31T23:51:58.359-08:00","display_name":"Teng Zhou","url":"https://pledco.academia.edu/TengZhou"},"attachments":[{"id":84351648,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351648/thumbnails/1.jpg","file_name":"micromachines-12-00744-v2.pdf","download_url":"https://www.academia.edu/attachments/84351648/download_file?st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&st=MTczMzAyNDI0MSw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Mixing_Mechanism_of_Microfluidic_Mixer_w.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351648/micromachines-12-00744-v2-libre.pdf?1650239166=\u0026response-content-disposition=attachment%3B+filename%3DMixing_Mechanism_of_Microfluidic_Mixer_w.pdf\u0026Expires=1733027841\u0026Signature=LEAQlYa0~muufOOJ5JeM6UAlLezmuf19tiYXIh4yc0sSYh2L52U2JjsWxnu5z3xtErMdpIi7YJWHGaBdDwqExz0m5KPS3MxgUUlJ1k8GMuxxpdINMEMM1x5iIvXAjLETlI15w4dLNvFQ8Xr44FBfD~Ao3ph83nAV8JYPdi81T87Q4zFS6sm9ohXx0com~VEz~8snlbOgg8aZfHIkgD8QoUMjEZVY4oDxsDvbUrsqLfUddRZhNvMsKqEhSEo8bam2cRNPninfHnDumPO8z9Dv2qdSODIB4KJLZJVC5anoYCbb1xfjsgxWpHXP-NU3C763YOZQfeCCux5LQp6GMZ58zw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":84351647,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84351647/thumbnails/1.jpg","file_name":"micromachines-12-00744-v2.pdf","download_url":"https://www.academia.edu/attachments/84351647/download_file","bulk_download_file_name":"Mixing_Mechanism_of_Microfluidic_Mixer_w.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84351647/micromachines-12-00744-v2-libre.pdf?1650239167=\u0026response-content-disposition=attachment%3B+filename%3DMixing_Mechanism_of_Microfluidic_Mixer_w.pdf\u0026Expires=1733027841\u0026Signature=L8aK-iYvSmd~nZvVZtMGxfYSya0H2pthZUtTftnJa-fvDnwiNoo0c1MNv2Xk2q95riLpUZA~1c2~3Z1glt2WNsP3wmu6cLXb44nJMxkzy-fO3kXKfI8trB57XL-TyYmSIDvv0HI~VdQn-kYurmDcPTZ~R5UOI1FaLj4N~DocN4ZMuLWT7a0uxxwUrRJrRH8g0rfKQT~N1Cc0gEnu4shEvtchLv8iz3GOsurKNqOkyeq0U-GemwJhuaSy9IsQAgeYMU1cYehKaA1k~0xjkUE4wqWkQc6dIL7ZCHUc89DfW4ObVZd9fGKrxYpNpwXEvPJvahsBXbXA3xFJiQW-wv9G8Q__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":26327,"name":"Medicine","url":"https://www.academia.edu/Documents/in/Medicine"}],"urls":[{"id":19595374,"url":"https://res.mdpi.com/d_attachment/micromachines/micromachines-12-00744/article_deploy/micromachines-12-00744-v2.pdf"}]}, dispatcherData: dispatcherData }); 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