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src="https://0.academia-photos.com/17085/5723/6794399/s200_prof._saeid.eslamian.jpg" /></a></div><div class="suggested-user-card__user-info"><a class="suggested-user-card__user-info__header ds2-5-body-sm-bold ds2-5-body-link" href="https://iut.academia.edu/ProfSaeidEslamian">Prof. Saeid Eslamian</a><p class="suggested-user-card__user-info__subheader ds2-5-body-xs">Isfahan University of Technology</p></div></div><div class="suggested-user-card"><div class="suggested-user-card__avatar social-profile-avatar-container"><a href="https://qub.academia.edu/JohnBarry"><img class="profile-avatar u-positionAbsolute" alt="John Barry" border="0" onerror="if (this.src != '//a.academia-assets.com/images/s200_no_pic.png') this.src = '//a.academia-assets.com/images/s200_no_pic.png';" width="200" height="200" src="https://0.academia-photos.com/31845/10282/2561912/s200_john.barry.jpg" /></a></div><div class="suggested-user-card__user-info"><a class="suggested-user-card__user-info__header 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class="profile-avatar u-positionAbsolute" alt="Mikail F Lumentut" border="0" onerror="if (this.src != '//a.academia-assets.com/images/s200_no_pic.png') this.src = '//a.academia-assets.com/images/s200_no_pic.png';" width="200" height="200" src="https://0.academia-photos.com/515230/269690/131913748/s200_mikail.lumentut.png" /></a></div><div class="suggested-user-card__user-info"><a class="suggested-user-card__user-info__header ds2-5-body-sm-bold ds2-5-body-link" href="https://taiwan.academia.edu/MikailLumentut">Mikail F Lumentut</a><p class="suggested-user-card__user-info__subheader ds2-5-body-xs">National Taiwan University</p></div></div><div class="suggested-user-card"><div class="suggested-user-card__avatar social-profile-avatar-container"><a href="https://usp-br.academia.edu/FernandoCatalano"><img class="profile-avatar u-positionAbsolute" alt="Fernando Catalano" border="0" onerror="if (this.src != '//a.academia-assets.com/images/s200_no_pic.png') this.src = 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class="profile--tab_heading_container">Papers by Farshid Chini</h3></div><div class="js-work-strip profile--work_container" data-work-id="115334270"><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/115334270/Slip_influence_on_a_blade_performance_under_different_pitch_oscillating_motion"><img alt="Research paper thumbnail of Slip influence on a blade performance under different pitch-oscillating motion" 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/115334270/Slip_influence_on_a_blade_performance_under_different_pitch_oscillating_motion">Slip influence on a blade performance under different pitch-oscillating motion</a></div><div class="wp-workCard_item"><span>Renewable and Sustainable Energy Reviews</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="115334270"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334270"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334270; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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href="https://www.academia.edu/115334269/Effect_of_Hydrophilic_and_Hydrophobic_Metal_Foams_on_Condensation_Characteristics_of_Refrigerant_Flow_Inside_Annular_Tubes_An_Experimental_Study"><img alt="Research paper thumbnail of Effect of Hydrophilic and Hydrophobic Metal Foams on Condensation Characteristics of Refrigerant Flow Inside Annular Tubes: An Experimental Study" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/115334269/Effect_of_Hydrophilic_and_Hydrophobic_Metal_Foams_on_Condensation_Characteristics_of_Refrigerant_Flow_Inside_Annular_Tubes_An_Experimental_Study">Effect of Hydrophilic and Hydrophobic Metal Foams on Condensation Characteristics of Refrigerant Flow Inside Annular Tubes: An Experimental Study</a></div><div class="wp-workCard_item"><span>Social Science Research Network</span><span>, 2022</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="115334269"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334269"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334269; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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})(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=115334269]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":115334269,"title":"Effect of Hydrophilic and Hydrophobic Metal Foams on Condensation Characteristics of Refrigerant Flow Inside Annular Tubes: An Experimental Study","internal_url":"https://www.academia.edu/115334269/Effect_of_Hydrophilic_and_Hydrophobic_Metal_Foams_on_Condensation_Characteristics_of_Refrigerant_Flow_Inside_Annular_Tubes_An_Experimental_Study","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="115334268"><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/115334268/Numerical_Investigation_of_Hydrodynamic_Forces_by_Imposing_Superhydrophobic_Slip_Boundary_Condition_on_Upper_and_Lower_Sides_of_Sd7003_Hydrofoil"><img alt="Research paper thumbnail of Numerical Investigation of Hydrodynamic Forces by Imposing Superhydrophobic Slip Boundary Condition on Upper and Lower Sides of Sd7003 Hydrofoil" class="work-thumbnail" src="https://attachments.academia-assets.com/111772314/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/115334268/Numerical_Investigation_of_Hydrodynamic_Forces_by_Imposing_Superhydrophobic_Slip_Boundary_Condition_on_Upper_and_Lower_Sides_of_Sd7003_Hydrofoil">Numerical Investigation of Hydrodynamic Forces by Imposing Superhydrophobic Slip Boundary Condition on Upper and Lower Sides of Sd7003 Hydrofoil</a></div><div class="wp-workCard_item"><span>Social Science Research Network</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">This article focuses on the steady motion of yawed planing hulls with emphasis on the effects 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">This article focuses on the steady motion of yawed planing hulls with emphasis on the effects of adding steps to the bottom of these vessels on the hydrodynamic forces and moments acting on the boat. To analyze the problem, the Ansys-CFX software is used and three different planing hulls are investigated in steady yawed condition. The main targeted results include hydrodynamic forces and moments acting on the boat at different yaw angles and beam Froude numbers which provide important insights regarding the effects of loading and adding step on these forces and moments. The numerically predicted sway forces are compared against experimental data, suggesting that the current numerical model predicts sway and surge forces with reasonable accuracy. Moreover, it is observed that surge force coefficient of the investigated prismatic planing hull with light loading condition does not change significantly when the hull is relocated in a yaw angle, while it is remarkably affected when the boat is heavy. Furthermore, it is observed that this prismatic planing hull has smaller rolling moment in a steady yawed motion, when it moves at larger beam Froude number. Meanwhile, the computed yawing moments of this hull indicate that an increase in speed does not change this moment notably, while an increase in its weight yields larger yawing moment. Comparison of the results of stepped and non-stepped planing hulls indicates that surge force coefficient of the stepped hull is larger, while its sway force and rolling moment are smaller. This is mainly caused by the shape of the interrupted wetted surface and larger number of maximum pressure area in the stepped planing hull. Finally, it is concluded that there is no significant difference between the yawing moment of the investigated stepped and non-stepped planing hulls.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ee296d031a99728284a73cbcfd19e6fe" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772314,"asset_id":115334268,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772314/download_file?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="115334268"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334268"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334268; 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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="115334267"><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/115334267/Using_genetic_algorithm_to_find_the_optimum_piecewise_superhydrophobic_pattern_maximizing_the_lift_to_drag_ratio_on_a_SD_7003_foil_at_different_working_conditions"><img alt="Research paper thumbnail of Using genetic algorithm to find the optimum piecewise superhydrophobic pattern maximizing the lift to drag ratio on a SD 7003 foil at different working conditions" 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/115334267/Using_genetic_algorithm_to_find_the_optimum_piecewise_superhydrophobic_pattern_maximizing_the_lift_to_drag_ratio_on_a_SD_7003_foil_at_different_working_conditions">Using genetic algorithm to find the optimum piecewise superhydrophobic pattern maximizing the lift to drag ratio on a SD 7003 foil at different working conditions</a></div><div class="wp-workCard_item"><span>Ocean Engineering</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="115334267"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334267"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334267; 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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=115334266]").text(description); $(".js-view-count[data-work-id=115334266]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 115334266; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='115334266']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=115334266]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":115334266,"title":"Numerical Analysis of Water Injection Effect on NOx Reduction of MGT-40 Gas Turbine","internal_url":"https://www.academia.edu/115334266/Numerical_Analysis_of_Water_Injection_Effect_on_NOx_Reduction_of_MGT_40_Gas_Turbine","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="115334265"><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/115334265/Electrokinetic_energy_conversion_in_a_finite_length_superhydrophobic_microchannel"><img alt="Research paper thumbnail of Electrokinetic energy conversion in a finite length superhydrophobic microchannel" class="work-thumbnail" src="https://attachments.academia-assets.com/111772313/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/115334265/Electrokinetic_energy_conversion_in_a_finite_length_superhydrophobic_microchannel">Electrokinetic energy conversion in a finite length superhydrophobic microchannel</a></div><div class="wp-workCard_item"><span>Chemical Physics Letters</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We investigated the effect of superhydrophobic walls on electrokinetics phenomena in a finite-len...</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">We investigated the effect of superhydrophobic walls on electrokinetics phenomena in a finite-length microchannel with superhydrophobic walls (in both transient and steady-state). We implemented the effect of superhydrophobicity using Navier's slip-length. To include the importance of the electric double-layer, we scaled the slip-length with respect to Debye-length (j À1). By increasing the sliplength from 0 to 144 nm (1.5j À1), streaming-current, streaming-potential, flow-rate and electrokinetic energy conversion increased by 2.55, 2.44, 1.8, and 3.4 folds, accordingly. The electrokinetic energy conversion of each microchannel was in the order of picowatt. To produce more energy, an array of microchannels should be used.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="27ccc8611bc1c2de9672873bcc058a29" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772313,"asset_id":115334265,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772313/download_file?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="115334265"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334265"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334265; 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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="115334179"><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/115334179/Design_and_fabrication_of_silicone_silica_nanocomposites_airway_stent"><img alt="Research paper thumbnail of Design and fabrication of silicone-silica nanocomposites airway stent" class="work-thumbnail" src="https://attachments.academia-assets.com/111772247/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/115334179/Design_and_fabrication_of_silicone_silica_nanocomposites_airway_stent">Design and fabrication of silicone-silica nanocomposites airway stent</a></div><div class="wp-workCard_item"><span>Frontiers in Materials</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Introduction: Due to the COVID-19 pandemic in recent years, many patients after extubation had st...</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">Introduction: Due to the COVID-19 pandemic in recent years, many patients after extubation had stenosis in all tracheal areas because of long-term intubation. Therefore, tracheal stenosis in these patients is benign and can be treated using silicone stents, and many patients need silicone stents during recovery. A silicone stent is an artificial support that plays a significant role in managing airway obstruction.Methods: This research aims to fabricate an optimal silicone stent reinforced with Nanosilica by vacuumed injection molding. Materials-based nanocomposites are made of rtv2 silicone with 1wt%, 3wt%, and 5wt% of hydrophilic and hydrophobic Nanosilica particles. Hardness, tensile, and hydrophobicity properties have been performed for the experimental characterization of the nanocomposites.Results and Discussion: The uniform distribution of nanoparticles in the silicone matrix has been confirmed using SEM images. Adding Nano-silica increases hardness and tensile strength and i...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5b7b7c52053b63827b32a864488e06c8" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772247,"asset_id":115334179,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772247/download_file?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="115334179"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334179"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334179; 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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="109917696"><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/109917696/Experiments_on_skin_friction_reduction_induced_by_superhydrophobicity_and_Leidenfrost_phenomena_in_a_Taylor_Couette_cell"><img alt="Research paper thumbnail of Experiments on skin friction reduction induced by superhydrophobicity and Leidenfrost phenomena in a Taylor-Couette cell" class="work-thumbnail" src="https://attachments.academia-assets.com/107897266/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/109917696/Experiments_on_skin_friction_reduction_induced_by_superhydrophobicity_and_Leidenfrost_phenomena_in_a_Taylor_Couette_cell">Experiments on skin friction reduction induced by superhydrophobicity and Leidenfrost phenomena in a Taylor-Couette cell</a></div><div class="wp-workCard_item"><span>International Journal of Heat and Mass Transfer</span><span>, 2019</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Film boiling and superhydrophobic surfaces may each decrease the skin drag by creating a vapor/ai...</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">Film boiling and superhydrophobic surfaces may each decrease the skin drag by creating a vapor/air layer encapsulating the body. However, film boiling requires enormous power, and air plastron on superhydrophobic surfaces is not stable. The combined utilization of superhydrophobicity and film boiling is promising as on superhydrophobic surfaces the film boiling (Leidenfrost) temperature is only a few degrees higher than the boiling point. In a recent literature, a Taylor-Couette (T-C) cell was proposed to measure the combined effect of superhydrophobicity and film boiling on skin drag. However, rotation of the inner cylinder of the TC cell creates turbulent Taylor vortices, makes the vapor layer unstable and creates uncertainty in the results. Whereas if the outer cylinder rotated, flow pattern would become azimuthal laminar with weak Ekman vortices. We modified the T-C cell, accordingly; and found that by decreasing the surface wettability (i.e. apparent contact angle), Leidenfrost temperature, and the minimum heat flux to reach the film boiling decrease as well. Furthermore, by increasing the shear Reynolds number from 0:8 Â 10 4 to 3:2 Â 10 4 , for both heated and unheated superhydrophobic surfaces, skin drag reduces. The heated one results in 67% decrease in skin drag. It is worth mentioning that the heat flux to create this 67% skin drag reduction is less than 2 W=cm 2 , which is 25 times less than the minimum heat flux to create film boiling on a regular aluminum surface.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="45639b6d5dab16036b5277e1446bacdd" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":107897266,"asset_id":109917696,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/107897266/download_file?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="109917696"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="109917696"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 109917696; 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$a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="80055440"><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/80055440/Studying_the_collapse_of_photoresist_patterns_during_photolithography_process"><img alt="Research paper thumbnail of Studying the collapse of photoresist patterns during photolithography process" class="work-thumbnail" src="https://attachments.academia-assets.com/86564306/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/80055440/Studying_the_collapse_of_photoresist_patterns_during_photolithography_process">Studying the collapse of photoresist patterns during photolithography process</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">NOTICE: The author has granted a nonexclusive license allowing Library and Archives Canada to rep...</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">NOTICE: The author has granted a nonexclusive license allowing Library and Archives Canada to reproduce, publish, archive, preserve, conserve, communicate to the public by telecommunication or on the Internet, loan, distribute and sell theses worldwide, for commercial or noncommercial purposes, in microform, paper, electronic and/or any other formats. AVIS: L'auteur a accorde une licence non exclusive permettant a la Bibliotheque et Archives Canada de reproduire, publier, archiver, sauvegarder, conserver, transmettre au public par telecommunication ou par Plntemet, prefer, distribuer et vendre des theses partout dans le monde, a des fins commerciales ou autres, sur support microforme, papier, electronique et/ou autres formats. Canada Bien que ces formulaires aient inclus dans la pagination, il n'y aura aucun contenu manquant.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b40871cfce3bc62312f9af0d3e58bb60" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":86564306,"asset_id":80055440,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/86564306/download_file?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="80055440"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="80055440"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 80055440; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b40871cfce3bc62312f9af0d3e58bb60" } } $('.js-work-strip[data-work-id=80055440]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":80055440,"title":"Studying the collapse of photoresist patterns during photolithography process","internal_url":"https://www.academia.edu/80055440/Studying_the_collapse_of_photoresist_patterns_during_photolithography_process","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[{"id":86564306,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/86564306/thumbnails/1.jpg","file_name":"MR45793.pdf","download_url":"https://www.academia.edu/attachments/86564306/download_file","bulk_download_file_name":"Studying_the_collapse_of_photoresist_pat.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/86564306/MR45793-libre.pdf?1653667593=\u0026response-content-disposition=attachment%3B+filename%3DStudying_the_collapse_of_photoresist_pat.pdf\u0026Expires=1740508180\u0026Signature=TW763ODvTwNagl4IqaCXCHO8jUZL0GwE0u9pr8961hKLQDGK8Ehvya2z1Y-DoBDq60VG7lS4Iv5tJVCZXtM0OIoibCNVK~QBm-goXitoATrPKONuZHeKxrCxrCo3ndHSIDkLmXwb6SxUldDWStzoollrUsz5rItW2UNpFRI8EvIifuKGFFMvaPYh3xBKLV4e12WMI7-xUJMQxf590OsylhX4D7GioWWoZJLktKLcddWh1Zr8qH5Nijvi~JqBsvIHmeS4T-2QjfDQyiqv-pqbtmd2zWKGmDgqahS4L3M4HBfkAiMfo0~BkkaWJ5uiNuy3V0TXemgT1Pso0-Sz1HjDWA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"},{"id":86564305,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/86564305/thumbnails/1.jpg","file_name":"MR45793.pdf","download_url":"https://www.academia.edu/attachments/86564305/download_file","bulk_download_file_name":"Studying_the_collapse_of_photoresist_pat.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/86564305/MR45793-libre.pdf?1653667617=\u0026response-content-disposition=attachment%3B+filename%3DStudying_the_collapse_of_photoresist_pat.pdf\u0026Expires=1740508181\u0026Signature=O8srksiDBn2apMm9wl-E7CBolklDHVTDq94e6tG2r3APjm4kJGuLsJROGR5b4hyp2wTFvtGd~QatB1LSD2cVxjbpILNPihIF2mQpKfz1mmPrU5hNSYOCljUtcT9Zk9W762W0rqxLYvMU-peAP-En7wph9Pbs5oDIdvs26pytKyHsCZhYxsF6H-DRL7XGoPaaK59CWp6DTinpGyPzp0trd70lWfObPlggSQKShWxRDv8X7lf6w4~WPTqV0otKx~CBby5-aPGlMW~spDU18tDkYpNu7lbZUxcOo6hNgm7qCK9EmYgVBbDl-mtFXGmBD8SsjNf5~NScW6kPRjVX3DK7uw__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}]}, 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="80055439"><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/80055439/Ionic_current_magnetic_fields_in_3D_finite_length_nanopores_and_nanoslits"><img alt="Research paper thumbnail of Ionic current magnetic fields in 3D finite-length nanopores and nanoslits" class="work-thumbnail" src="https://attachments.academia-assets.com/86564304/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/80055439/Ionic_current_magnetic_fields_in_3D_finite_length_nanopores_and_nanoslits">Ionic current magnetic fields in 3D finite-length nanopores and nanoslits</a></div><div class="wp-workCard_item"><span>The European Physical Journal Plus</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Deoxyribonucleic acid (DNA) encodes all genetic information, and in genetic disorders, DNA sequen...</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">Deoxyribonucleic acid (DNA) encodes all genetic information, and in genetic disorders, DNA sequencing is used as an effective diagnosis. Nanopore/slit is one of the recent and successful tools for DNA sequencing. Passage of DNA along the pores creates non-uniform ionic currents which creates non-uniform electric and magnetic fields, accordingly. Sensing the electric field is usually used for sequencing application. We suggest to use the magnetic field induced by pressure-driven ionic currents as a secondary signal. We systematically compared the induced magnetic field of nanopores and nanoslits with equal cross-sectional area. The 3D magnetic field is numerically obtained by solving the Poisson-Nernst-Planck, Ampere, and Navier-Stokes equations. As expected, the maximum value of the maximum magnetic flux occurs near the wall and inside the channel, and increasing the pressure gradient along the pore/slit increases the flowrate and magnetic field, consequently. At a given pressure difference across the pore/slit, nanopores are better than nanoslits in sensing the magnetic flux. For example, by applying 2 MPa across the pore/slit, the maximum magnetic flux density for nanopore, nanoslit AR 1 and nanoslit AR 5 are 1.10 pT, 1.08 pT and 0.45 pT, accordingly. Also, at a given flowrate across the pore/slit, nanoslits are the better choice. It should be noted the external magnetic fields as small as pico-Tesla are detectable and measurable in voltage/pressure driven electrokinetic flow slits.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63bbde09c138f0bf2f1f11dda0cd872b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":86564304,"asset_id":80055439,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/86564304/download_file?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="80055439"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="80055439"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 80055439; 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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="73110184"><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/73110184/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD7003_Foil_A_Numerical_Approach"><img alt="Research paper thumbnail of Effect of Superhydrophobic Surface on Drag Coefficient of SD7003 Foil: A Numerical Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81760181/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/73110184/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD7003_Foil_A_Numerical_Approach">Effect of Superhydrophobic Surface on Drag Coefficient of SD7003 Foil: A Numerical Approach</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">‫مجله‬ ‫مدرس‬ ‫مکانیک‬ ‫مهندسی‬ ، ‫اردیبهشت‬ 9316 ‫دوره‬ ، 91 ‫شماره‬ ، 2 ‫ص‬ ، ‫ص‬ 926-934 ‫ماهن...</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">‫مجله‬ ‫مدرس‬ ‫مکانیک‬ ‫مهندسی‬ ، ‫اردیبهشت‬ 9316 ‫دوره‬ ، 91 ‫شماره‬ ، 2 ‫ص‬ ، ‫ص‬ 926-934 ‫ماهنامه‬ ‫پژوهشی‬ ‫علمی‬ ‫مهندسی‬ ‫مکانیک‬ ‫مدرس‬ mme.modares.ac.ir ‫نمایید‬ ‫استفاده‬ ‫ذیل‬ ‫عبارت‬ ‫از‬ ‫مقاله‬ ‫این‬ ‫به‬ ‫ارجاع‬ ‫برای‬ : Please cite this article using: Due to low surface energy and hierarchical roughness, fluids on superhydrophobic surfaces are mobile. The slip velocity on these surfaces is formulated using Navier&#39;s slip length. On regular surfaces, slip length is only a few nano-meters. On superhydrophobic surfaces, slip length can be as large as 500 µm. Literature studies usually make the entire surface superhydrophobic which may not be the optimum situation. To find the desirable regions, the problem should be analyzed numerically. Most of the numerical studies are for flat plates. On curved surfaces (e.g. foils), due to the adverse pressure gradient and possibility of separation, analysis is more complicated. Here, the effect of using superhydrophobic surface f...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="66fe3c746b9f4a8491ca80a4761b2ff9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81760181,"asset_id":73110184,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81760181/download_file?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="73110184"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="73110184"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 73110184; 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</script> <div class="js-work-strip profile--work_container" data-work-id="72278836"><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/72278836/Numerical_simulation_of_droplet_impact_on_vibrating_low_adhesion_surfaces"><img alt="Research paper thumbnail of Numerical simulation of droplet impact on vibrating low-adhesion surfaces" 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/72278836/Numerical_simulation_of_droplet_impact_on_vibrating_low_adhesion_surfaces">Numerical simulation of droplet impact on vibrating low-adhesion surfaces</a></div><div class="wp-workCard_item"><span>Physics of Fluids</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The impact of droplets on low-adhesion solid surfaces vibrating in the vertical direction was num...</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 impact of droplets on low-adhesion solid surfaces vibrating in the vertical direction was numerically investigated. An axisymmetric multiphase lattice Boltzmann model capable of handling high density and viscosity ratios was implemented to simulate the impact. The effects of vibration parameters on the spreading, contact time, and droplet rebound velocity were addressed. According to the results, the phase angle of the surface vibration is the most dominant factor in determining the dynamics of the droplet upon impact. The contact time generally increases when the surface is vibrated. However, for a certain range of phase angles, the contact time can decrease, as compared to the stationary surface. The rebound velocity also shows a strong dependence on the vibration frequency and phase angle. For droplets with higher impact velocities, the surface vibration becomes a less important factor, whereas on surfaces with lower contact angles, the impact dynamics are much more heavily affected by the surface vibration. The rebound velocity is also heavily affected by surface vibration and varies depending on the frequency and phase angle. This study offers insights into the physics of droplet impact upon vibrating surfaces, which can be utilized to improve surface wettability control in applications where vibration is present.</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="72278836"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278836"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278836; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72278835]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72278835,"title":"The Potential of Surface Nano‐Engineering and Superhydrophobic Surfaces in Drag Reduction","internal_url":"https://www.academia.edu/72278835/The_Potential_of_Surface_Nano_Engineering_and_Superhydrophobic_Surfaces_in_Drag_Reduction","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="72278833"><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/72278833/Sessile_and_Pendant_Micro_Liter_Drops_Evaporate_at_Different_Rates_An_Experimental_Approach"><img alt="Research paper thumbnail of Sessile and Pendant Micro-Liter Drops Evaporate at Different Rates: An Experimental Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269273/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/72278833/Sessile_and_Pendant_Micro_Liter_Drops_Evaporate_at_Different_Rates_An_Experimental_Approach">Sessile and Pendant Micro-Liter Drops Evaporate at Different Rates: An Experimental Approach</a></div><div class="wp-workCard_item"><span>Applied and Computational Mechanics</span><span>, 2016</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Evaporation of micro-liter drops from solid surfaces at room condition is mainly governed by diff...</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">Evaporation of micro-liter drops from solid surfaces at room condition is mainly governed by diffusion. Therefore, there should be no difference between evaporation rate of sessile and pendant drops. However, some studies indicate a difference and explain the difference using buoyancy. The objective here is to reconcile the inconsistency in the literature. For that, first, by comparing two identical suspended drops, one with a plate on top and the other underneath with a space between drop and plate, we showed the contribution of buoyancy in evaporation is at most less than 8%. When a plate was placed on top, water (its vapor is lighter than air) evaporated slower and hydrocarbons (their vapors are heavier than air) evaporated faster. Interestingly, it was observed when drops touch the plates (i.e. sessile and pendant drops), both water and hydrocarbon drops evaporated faster in sessile configuration. The observation for hydrocarbons is in contradiction with what buoyancy explains. ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b38ee6235bfad7294ab09601dc19e131" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269273,"asset_id":72278833,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269273/download_file?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="72278833"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278833"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278833; 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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="72278832"><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/72278832/Improving_the_natural_convective_heat_transfer_of_a_rectangular_heatsink_using_superhydrophobic_walls_A_numerical_approach"><img alt="Research paper thumbnail of Improving the natural convective heat transfer of a rectangular heatsink using superhydrophobic walls: A numerical approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269274/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/72278832/Improving_the_natural_convective_heat_transfer_of_a_rectangular_heatsink_using_superhydrophobic_walls_A_numerical_approach">Improving the natural convective heat transfer of a rectangular heatsink using superhydrophobic walls: A numerical approach</a></div><div class="wp-workCard_item"><span>Environmental Engineering Science</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The effect of utilizing superhydrophobic walls on improving the convective heat transfer in a rec...</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 effect of utilizing superhydrophobic walls on improving the convective heat transfer in a rectangular heatsink has been studied numerically in this paper. The vertical walls were kept at isothermal hot-and-cold temperatures and horizontal walls were insulated. The boundary condition on the walls was: no-slip for regular, and slip (with slip length of 500 µm) for superhydrophobic walls. By changing the heatsink aspect ratio (AR, height/width) from 0.1 to 10, it was observed that regardless of the wall slip, the optimum AR is 1, i.e. square enclosure. For a square heatsink, using the nanofluid with = 3% could enhance the heat transfer (quantified by Nusselt number) by up to 9.8%. For the same enclosure filled with pure water, applying superhydrophobic horizontal walls could increase the heat transfer by 4.45%. The joint effect of using superhydrophobic walls and nano-particles enhanced the heat transfer by up to 14.75%. The results of this paper may open a new avenue for high per...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="beadfe4d4a78fb3653b0937c66ff35de" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269274,"asset_id":72278832,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269274/download_file?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="72278832"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278832"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278832; 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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="72278831"><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/72278831/A_Diffusive_Model_for_Evaporation_of_Spherical_Water_Drops_at_Room_Temperature_and_Standard_Pressure"><img alt="Research paper thumbnail of A Diffusive Model for Evaporation of Spherical Water Drops at Room Temperature and Standard Pressure" class="work-thumbnail" src="https://attachments.academia-assets.com/81269270/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/72278831/A_Diffusive_Model_for_Evaporation_of_Spherical_Water_Drops_at_Room_Temperature_and_Standard_Pressure">A Diffusive Model for Evaporation of Spherical Water Drops at Room Temperature and Standard Pressure</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Evaporation of drops at room temperature and atmospheric conditions is mainly impelled by diffusi...</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">Evaporation of drops at room temperature and atmospheric conditions is mainly impelled by diffusion of vapor. Diffusion of vapor is a function of vapor concentration gradient (VCG) at the drop surface. The developed model in this paper modifies the relations used for finding the VCG for drops. The relations in literature for evaporation of millimetric drops are based on the study of Maxwell, which was originally for evaporation from a wet bulb. The VCG according to Maxwell based models is stationary and a function of the inverse of the bulb radius. However, where one uses this model for millimetric drops, the VCG becomes time dependent and increases in time (as during the evaporation, drop radius decreases). Intuitively it is understandable that the VCG should decrease in time (notwithstanding the Kelvin effect for very small microscopic drops). In this study a diffusion model is developed which uses a time dependent VCG that decreases in time. The developed diffusion model is able ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="01d1712312456ab0d3563c7119be8d67" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269270,"asset_id":72278831,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269270/download_file?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="72278831"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278831"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278831; 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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="72278830"><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/72278830/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD_7003_Foil_A_Numerical_Approach"><img alt="Research paper thumbnail of Effect of Superhydrophobic Surface on Drag Coefficient of SD 7003 Foil : A Numerical Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269268/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/72278830/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD_7003_Foil_A_Numerical_Approach">Effect of Superhydrophobic Surface on Drag Coefficient of SD 7003 Foil : A Numerical Approach</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">هلاقم تاعلاطا هدیکچ لهبک یطٍّظپ ِلبقه :تفبیسد 28 شْه 1395 :ششیزپ 21 سرآ 1395 :تیبس سد ِئاسا 91 يو...</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">هلاقم تاعلاطا هدیکچ لهبک یطٍّظپ ِلبقه :تفبیسد 28 شْه 1395 :ششیزپ 21 سرآ 1395 :تیبس سد ِئاسا 91 يوْث 9911 ِث یطشًا تلع یساَوّبً دَجٍ ٍ نک یحطس ةآ قَف حَطس یٍس شث لبیس ،ًَبً دبعثا سد بّ یه ضیشگ لَط صا شضغل يیا ىداد ىبطً یاشث .دضغل یه ُدبفتسا شیٍبً شضغل ًَبً ذٌچ دٍذح سد شضغل لَط یلَ وعه حَطس یاشث .دَض قَف حَطس یاشث یلٍ ،تسا شته یه ضیشگثآ بت ذًاَت μm 500 نّ اٍاشف تبعلبطه .ذسشث مبجًا بسپ یٍشیً شث ىآ شثا ٍ شضغل لَط یٍس شث یً ةآ قَف حطس لک ًلاَوعه تبعلبطه يیا سد .تسا ُذض یه ضیشگ .ددشگ شٍس ٌِیْث یحاَ ً يتفبی یاشث یه یدذع یبّ صیث یدذع تبعلبطه یلٍ ذضبث ذیفه ذًاَت یه تخت حَطس یٍس شث شت یٌحٌه حَطس یٍس شث .ذٌضبث لیَف ذًٌبه( یه ُذیچیپ ِلئسه یسسشث )صیاذج ىذهآ دَجٍ ِث ىبکها ٍ( یفٌه سبطف ىبیداشگ دَجٍ لیلد ِث )بّ ِث ِلبقه يیا سد .دَض یدذع تسَص لیَفٍسذیّ شضغل لَط شیثأت یسسشث ِث SD7003 صذلٌَیس سد تِخادشپ فلتخه یبّ .تسا ُذض نّ ٍ شیزپبً نکاشت ،ماسآ ىبیشج ِتفشگ شظً سد بهد شتٍ لَط بث مَیٌیهَلآ سٌج صا لیَفٍسذیّ ٍ ُذض cm 10 ةبختًا طشض ٍد سد بسپ تیشض ٍ سبطف تیشض ،یضشث صٌت تیشض جیبتً .تسا ُذض ُذض ِسیبقه شگیذکی...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="46ad7e7466129271220b8404c3840ed9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269268,"asset_id":72278830,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269268/download_file?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="72278830"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278830"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278830; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="13427346" id="papers"><div class="js-work-strip profile--work_container" data-work-id="115334270"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/115334270/Slip_influence_on_a_blade_performance_under_different_pitch_oscillating_motion"><img alt="Research paper thumbnail of Slip influence on a blade performance under different pitch-oscillating motion" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/115334270/Slip_influence_on_a_blade_performance_under_different_pitch_oscillating_motion">Slip influence on a blade performance under different pitch-oscillating motion</a></div><div class="wp-workCard_item"><span>Renewable and Sustainable Energy Reviews</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="115334270"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334270"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334270; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=115334270]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":115334270,"title":"Slip influence on a blade performance under different pitch-oscillating motion","internal_url":"https://www.academia.edu/115334270/Slip_influence_on_a_blade_performance_under_different_pitch_oscillating_motion","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="115334269"><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/115334269/Effect_of_Hydrophilic_and_Hydrophobic_Metal_Foams_on_Condensation_Characteristics_of_Refrigerant_Flow_Inside_Annular_Tubes_An_Experimental_Study"><img alt="Research paper thumbnail of Effect of Hydrophilic and Hydrophobic Metal Foams on Condensation Characteristics of Refrigerant Flow Inside Annular Tubes: An Experimental Study" 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/115334269/Effect_of_Hydrophilic_and_Hydrophobic_Metal_Foams_on_Condensation_Characteristics_of_Refrigerant_Flow_Inside_Annular_Tubes_An_Experimental_Study">Effect of Hydrophilic and Hydrophobic Metal Foams on Condensation Characteristics of Refrigerant Flow Inside Annular Tubes: An Experimental Study</a></div><div class="wp-workCard_item"><span>Social Science Research Network</span><span>, 2022</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="115334269"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334269"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334269; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=115334269]").text(description); $(".js-view-count[data-work-id=115334269]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 115334269; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='115334269']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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); 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} }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="115334268"><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/115334268/Numerical_Investigation_of_Hydrodynamic_Forces_by_Imposing_Superhydrophobic_Slip_Boundary_Condition_on_Upper_and_Lower_Sides_of_Sd7003_Hydrofoil"><img alt="Research paper thumbnail of Numerical Investigation of Hydrodynamic Forces by Imposing Superhydrophobic Slip Boundary Condition on Upper and Lower Sides of Sd7003 Hydrofoil" class="work-thumbnail" src="https://attachments.academia-assets.com/111772314/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/115334268/Numerical_Investigation_of_Hydrodynamic_Forces_by_Imposing_Superhydrophobic_Slip_Boundary_Condition_on_Upper_and_Lower_Sides_of_Sd7003_Hydrofoil">Numerical Investigation of Hydrodynamic Forces by Imposing Superhydrophobic Slip Boundary Condition on Upper and Lower Sides of Sd7003 Hydrofoil</a></div><div class="wp-workCard_item"><span>Social Science Research Network</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">This article focuses on the steady motion of yawed planing hulls with emphasis on the effects 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">This article focuses on the steady motion of yawed planing hulls with emphasis on the effects of adding steps to the bottom of these vessels on the hydrodynamic forces and moments acting on the boat. To analyze the problem, the Ansys-CFX software is used and three different planing hulls are investigated in steady yawed condition. The main targeted results include hydrodynamic forces and moments acting on the boat at different yaw angles and beam Froude numbers which provide important insights regarding the effects of loading and adding step on these forces and moments. The numerically predicted sway forces are compared against experimental data, suggesting that the current numerical model predicts sway and surge forces with reasonable accuracy. Moreover, it is observed that surge force coefficient of the investigated prismatic planing hull with light loading condition does not change significantly when the hull is relocated in a yaw angle, while it is remarkably affected when the boat is heavy. Furthermore, it is observed that this prismatic planing hull has smaller rolling moment in a steady yawed motion, when it moves at larger beam Froude number. Meanwhile, the computed yawing moments of this hull indicate that an increase in speed does not change this moment notably, while an increase in its weight yields larger yawing moment. Comparison of the results of stepped and non-stepped planing hulls indicates that surge force coefficient of the stepped hull is larger, while its sway force and rolling moment are smaller. This is mainly caused by the shape of the interrupted wetted surface and larger number of maximum pressure area in the stepped planing hull. Finally, it is concluded that there is no significant difference between the yawing moment of the investigated stepped and non-stepped planing hulls.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ee296d031a99728284a73cbcfd19e6fe" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772314,"asset_id":115334268,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772314/download_file?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="115334268"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334268"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334268; 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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=115334266]").text(description); $(".js-view-count[data-work-id=115334266]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 115334266; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='115334266']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=115334266]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":115334266,"title":"Numerical Analysis of Water Injection Effect on NOx Reduction of MGT-40 Gas Turbine","internal_url":"https://www.academia.edu/115334266/Numerical_Analysis_of_Water_Injection_Effect_on_NOx_Reduction_of_MGT_40_Gas_Turbine","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="115334265"><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/115334265/Electrokinetic_energy_conversion_in_a_finite_length_superhydrophobic_microchannel"><img alt="Research paper thumbnail of Electrokinetic energy conversion in a finite length superhydrophobic microchannel" class="work-thumbnail" src="https://attachments.academia-assets.com/111772313/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/115334265/Electrokinetic_energy_conversion_in_a_finite_length_superhydrophobic_microchannel">Electrokinetic energy conversion in a finite length superhydrophobic microchannel</a></div><div class="wp-workCard_item"><span>Chemical Physics Letters</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We investigated the effect of superhydrophobic walls on electrokinetics phenomena in a finite-len...</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">We investigated the effect of superhydrophobic walls on electrokinetics phenomena in a finite-length microchannel with superhydrophobic walls (in both transient and steady-state). We implemented the effect of superhydrophobicity using Navier's slip-length. To include the importance of the electric double-layer, we scaled the slip-length with respect to Debye-length (j À1). By increasing the sliplength from 0 to 144 nm (1.5j À1), streaming-current, streaming-potential, flow-rate and electrokinetic energy conversion increased by 2.55, 2.44, 1.8, and 3.4 folds, accordingly. The electrokinetic energy conversion of each microchannel was in the order of picowatt. To produce more energy, an array of microchannels should be used.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="27ccc8611bc1c2de9672873bcc058a29" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772313,"asset_id":115334265,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772313/download_file?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="115334265"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334265"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334265; 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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="115334179"><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/115334179/Design_and_fabrication_of_silicone_silica_nanocomposites_airway_stent"><img alt="Research paper thumbnail of Design and fabrication of silicone-silica nanocomposites airway stent" class="work-thumbnail" src="https://attachments.academia-assets.com/111772247/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/115334179/Design_and_fabrication_of_silicone_silica_nanocomposites_airway_stent">Design and fabrication of silicone-silica nanocomposites airway stent</a></div><div class="wp-workCard_item"><span>Frontiers in Materials</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Introduction: Due to the COVID-19 pandemic in recent years, many patients after extubation had st...</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">Introduction: Due to the COVID-19 pandemic in recent years, many patients after extubation had stenosis in all tracheal areas because of long-term intubation. Therefore, tracheal stenosis in these patients is benign and can be treated using silicone stents, and many patients need silicone stents during recovery. A silicone stent is an artificial support that plays a significant role in managing airway obstruction.Methods: This research aims to fabricate an optimal silicone stent reinforced with Nanosilica by vacuumed injection molding. Materials-based nanocomposites are made of rtv2 silicone with 1wt%, 3wt%, and 5wt% of hydrophilic and hydrophobic Nanosilica particles. Hardness, tensile, and hydrophobicity properties have been performed for the experimental characterization of the nanocomposites.Results and Discussion: The uniform distribution of nanoparticles in the silicone matrix has been confirmed using SEM images. Adding Nano-silica increases hardness and tensile strength and i...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5b7b7c52053b63827b32a864488e06c8" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":111772247,"asset_id":115334179,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/111772247/download_file?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="115334179"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="115334179"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 115334179; 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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="109917696"><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/109917696/Experiments_on_skin_friction_reduction_induced_by_superhydrophobicity_and_Leidenfrost_phenomena_in_a_Taylor_Couette_cell"><img alt="Research paper thumbnail of Experiments on skin friction reduction induced by superhydrophobicity and Leidenfrost phenomena in a Taylor-Couette cell" class="work-thumbnail" src="https://attachments.academia-assets.com/107897266/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/109917696/Experiments_on_skin_friction_reduction_induced_by_superhydrophobicity_and_Leidenfrost_phenomena_in_a_Taylor_Couette_cell">Experiments on skin friction reduction induced by superhydrophobicity and Leidenfrost phenomena in a Taylor-Couette cell</a></div><div class="wp-workCard_item"><span>International Journal of Heat and Mass Transfer</span><span>, 2019</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Film boiling and superhydrophobic surfaces may each decrease the skin drag by creating a vapor/ai...</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">Film boiling and superhydrophobic surfaces may each decrease the skin drag by creating a vapor/air layer encapsulating the body. However, film boiling requires enormous power, and air plastron on superhydrophobic surfaces is not stable. The combined utilization of superhydrophobicity and film boiling is promising as on superhydrophobic surfaces the film boiling (Leidenfrost) temperature is only a few degrees higher than the boiling point. In a recent literature, a Taylor-Couette (T-C) cell was proposed to measure the combined effect of superhydrophobicity and film boiling on skin drag. However, rotation of the inner cylinder of the TC cell creates turbulent Taylor vortices, makes the vapor layer unstable and creates uncertainty in the results. Whereas if the outer cylinder rotated, flow pattern would become azimuthal laminar with weak Ekman vortices. We modified the T-C cell, accordingly; and found that by decreasing the surface wettability (i.e. apparent contact angle), Leidenfrost temperature, and the minimum heat flux to reach the film boiling decrease as well. Furthermore, by increasing the shear Reynolds number from 0:8 Â 10 4 to 3:2 Â 10 4 , for both heated and unheated superhydrophobic surfaces, skin drag reduces. The heated one results in 67% decrease in skin drag. It is worth mentioning that the heat flux to create this 67% skin drag reduction is less than 2 W=cm 2 , which is 25 times less than the minimum heat flux to create film boiling on a regular aluminum surface.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="45639b6d5dab16036b5277e1446bacdd" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":107897266,"asset_id":109917696,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/107897266/download_file?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="109917696"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="109917696"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 109917696; 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$a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="80055440"><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/80055440/Studying_the_collapse_of_photoresist_patterns_during_photolithography_process"><img alt="Research paper thumbnail of Studying the collapse of photoresist patterns during photolithography process" class="work-thumbnail" src="https://attachments.academia-assets.com/86564306/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/80055440/Studying_the_collapse_of_photoresist_patterns_during_photolithography_process">Studying the collapse of photoresist patterns during photolithography process</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">NOTICE: The author has granted a nonexclusive license allowing Library and Archives Canada to rep...</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">NOTICE: The author has granted a nonexclusive license allowing Library and Archives Canada to reproduce, publish, archive, preserve, conserve, communicate to the public by telecommunication or on the Internet, loan, distribute and sell theses worldwide, for commercial or noncommercial purposes, in microform, paper, electronic and/or any other formats. AVIS: L'auteur a accorde une licence non exclusive permettant a la Bibliotheque et Archives Canada de reproduire, publier, archiver, sauvegarder, conserver, transmettre au public par telecommunication ou par Plntemet, prefer, distribuer et vendre des theses partout dans le monde, a des fins commerciales ou autres, sur support microforme, papier, electronique et/ou autres formats. Canada Bien que ces formulaires aient inclus dans la pagination, il n'y aura aucun contenu manquant.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b40871cfce3bc62312f9af0d3e58bb60" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":86564306,"asset_id":80055440,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/86564306/download_file?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="80055440"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="80055440"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 80055440; 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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="80055439"><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/80055439/Ionic_current_magnetic_fields_in_3D_finite_length_nanopores_and_nanoslits"><img alt="Research paper thumbnail of Ionic current magnetic fields in 3D finite-length nanopores and nanoslits" class="work-thumbnail" src="https://attachments.academia-assets.com/86564304/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/80055439/Ionic_current_magnetic_fields_in_3D_finite_length_nanopores_and_nanoslits">Ionic current magnetic fields in 3D finite-length nanopores and nanoslits</a></div><div class="wp-workCard_item"><span>The European Physical Journal Plus</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Deoxyribonucleic acid (DNA) encodes all genetic information, and in genetic disorders, DNA sequen...</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">Deoxyribonucleic acid (DNA) encodes all genetic information, and in genetic disorders, DNA sequencing is used as an effective diagnosis. Nanopore/slit is one of the recent and successful tools for DNA sequencing. Passage of DNA along the pores creates non-uniform ionic currents which creates non-uniform electric and magnetic fields, accordingly. Sensing the electric field is usually used for sequencing application. We suggest to use the magnetic field induced by pressure-driven ionic currents as a secondary signal. We systematically compared the induced magnetic field of nanopores and nanoslits with equal cross-sectional area. The 3D magnetic field is numerically obtained by solving the Poisson-Nernst-Planck, Ampere, and Navier-Stokes equations. As expected, the maximum value of the maximum magnetic flux occurs near the wall and inside the channel, and increasing the pressure gradient along the pore/slit increases the flowrate and magnetic field, consequently. At a given pressure difference across the pore/slit, nanopores are better than nanoslits in sensing the magnetic flux. For example, by applying 2 MPa across the pore/slit, the maximum magnetic flux density for nanopore, nanoslit AR 1 and nanoslit AR 5 are 1.10 pT, 1.08 pT and 0.45 pT, accordingly. Also, at a given flowrate across the pore/slit, nanoslits are the better choice. It should be noted the external magnetic fields as small as pico-Tesla are detectable and measurable in voltage/pressure driven electrokinetic flow slits.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63bbde09c138f0bf2f1f11dda0cd872b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":86564304,"asset_id":80055439,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/86564304/download_file?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="80055439"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="80055439"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 80055439; 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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="73110184"><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/73110184/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD7003_Foil_A_Numerical_Approach"><img alt="Research paper thumbnail of Effect of Superhydrophobic Surface on Drag Coefficient of SD7003 Foil: A Numerical Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81760181/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/73110184/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD7003_Foil_A_Numerical_Approach">Effect of Superhydrophobic Surface on Drag Coefficient of SD7003 Foil: A Numerical Approach</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">‫مجله‬ ‫مدرس‬ ‫مکانیک‬ ‫مهندسی‬ ، ‫اردیبهشت‬ 9316 ‫دوره‬ ، 91 ‫شماره‬ ، 2 ‫ص‬ ، ‫ص‬ 926-934 ‫ماهن...</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">‫مجله‬ ‫مدرس‬ ‫مکانیک‬ ‫مهندسی‬ ، ‫اردیبهشت‬ 9316 ‫دوره‬ ، 91 ‫شماره‬ ، 2 ‫ص‬ ، ‫ص‬ 926-934 ‫ماهنامه‬ ‫پژوهشی‬ ‫علمی‬ ‫مهندسی‬ ‫مکانیک‬ ‫مدرس‬ mme.modares.ac.ir ‫نمایید‬ ‫استفاده‬ ‫ذیل‬ ‫عبارت‬ ‫از‬ ‫مقاله‬ ‫این‬ ‫به‬ ‫ارجاع‬ ‫برای‬ : Please cite this article using: Due to low surface energy and hierarchical roughness, fluids on superhydrophobic surfaces are mobile. The slip velocity on these surfaces is formulated using Navier&#39;s slip length. On regular surfaces, slip length is only a few nano-meters. On superhydrophobic surfaces, slip length can be as large as 500 µm. Literature studies usually make the entire surface superhydrophobic which may not be the optimum situation. To find the desirable regions, the problem should be analyzed numerically. Most of the numerical studies are for flat plates. On curved surfaces (e.g. foils), due to the adverse pressure gradient and possibility of separation, analysis is more complicated. Here, the effect of using superhydrophobic surface f...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="66fe3c746b9f4a8491ca80a4761b2ff9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81760181,"asset_id":73110184,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81760181/download_file?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="73110184"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="73110184"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 73110184; 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</script> <div class="js-work-strip profile--work_container" data-work-id="72278836"><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/72278836/Numerical_simulation_of_droplet_impact_on_vibrating_low_adhesion_surfaces"><img alt="Research paper thumbnail of Numerical simulation of droplet impact on vibrating low-adhesion surfaces" 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/72278836/Numerical_simulation_of_droplet_impact_on_vibrating_low_adhesion_surfaces">Numerical simulation of droplet impact on vibrating low-adhesion surfaces</a></div><div class="wp-workCard_item"><span>Physics of Fluids</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The impact of droplets on low-adhesion solid surfaces vibrating in the vertical direction was num...</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 impact of droplets on low-adhesion solid surfaces vibrating in the vertical direction was numerically investigated. An axisymmetric multiphase lattice Boltzmann model capable of handling high density and viscosity ratios was implemented to simulate the impact. The effects of vibration parameters on the spreading, contact time, and droplet rebound velocity were addressed. According to the results, the phase angle of the surface vibration is the most dominant factor in determining the dynamics of the droplet upon impact. The contact time generally increases when the surface is vibrated. However, for a certain range of phase angles, the contact time can decrease, as compared to the stationary surface. The rebound velocity also shows a strong dependence on the vibration frequency and phase angle. For droplets with higher impact velocities, the surface vibration becomes a less important factor, whereas on surfaces with lower contact angles, the impact dynamics are much more heavily affected by the surface vibration. The rebound velocity is also heavily affected by surface vibration and varies depending on the frequency and phase angle. This study offers insights into the physics of droplet impact upon vibrating surfaces, which can be utilized to improve surface wettability control in applications where vibration is present.</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="72278836"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278836"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278836; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72278835]").text(description); $(".js-view-count[data-work-id=72278835]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72278835; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72278835']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=72278835]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72278835,"title":"The Potential of Surface Nano‐Engineering and Superhydrophobic Surfaces in Drag Reduction","internal_url":"https://www.academia.edu/72278835/The_Potential_of_Surface_Nano_Engineering_and_Superhydrophobic_Surfaces_in_Drag_Reduction","owner_id":73827648,"coauthors_can_edit":true,"owner":{"id":73827648,"first_name":"Farshid","middle_initials":null,"last_name":"Chini","page_name":"ChiniF","domain_name":"independent","created_at":"2018-01-07T23:04:36.324-08:00","display_name":"Farshid Chini","url":"https://independent.academia.edu/ChiniF"},"attachments":[]}, 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="72278833"><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/72278833/Sessile_and_Pendant_Micro_Liter_Drops_Evaporate_at_Different_Rates_An_Experimental_Approach"><img alt="Research paper thumbnail of Sessile and Pendant Micro-Liter Drops Evaporate at Different Rates: An Experimental Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269273/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/72278833/Sessile_and_Pendant_Micro_Liter_Drops_Evaporate_at_Different_Rates_An_Experimental_Approach">Sessile and Pendant Micro-Liter Drops Evaporate at Different Rates: An Experimental Approach</a></div><div class="wp-workCard_item"><span>Applied and Computational Mechanics</span><span>, 2016</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Evaporation of micro-liter drops from solid surfaces at room condition is mainly governed by diff...</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">Evaporation of micro-liter drops from solid surfaces at room condition is mainly governed by diffusion. Therefore, there should be no difference between evaporation rate of sessile and pendant drops. However, some studies indicate a difference and explain the difference using buoyancy. The objective here is to reconcile the inconsistency in the literature. For that, first, by comparing two identical suspended drops, one with a plate on top and the other underneath with a space between drop and plate, we showed the contribution of buoyancy in evaporation is at most less than 8%. When a plate was placed on top, water (its vapor is lighter than air) evaporated slower and hydrocarbons (their vapors are heavier than air) evaporated faster. Interestingly, it was observed when drops touch the plates (i.e. sessile and pendant drops), both water and hydrocarbon drops evaporated faster in sessile configuration. The observation for hydrocarbons is in contradiction with what buoyancy explains. ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b38ee6235bfad7294ab09601dc19e131" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269273,"asset_id":72278833,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269273/download_file?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="72278833"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278833"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278833; 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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="72278832"><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/72278832/Improving_the_natural_convective_heat_transfer_of_a_rectangular_heatsink_using_superhydrophobic_walls_A_numerical_approach"><img alt="Research paper thumbnail of Improving the natural convective heat transfer of a rectangular heatsink using superhydrophobic walls: A numerical approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269274/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/72278832/Improving_the_natural_convective_heat_transfer_of_a_rectangular_heatsink_using_superhydrophobic_walls_A_numerical_approach">Improving the natural convective heat transfer of a rectangular heatsink using superhydrophobic walls: A numerical approach</a></div><div class="wp-workCard_item"><span>Environmental Engineering Science</span><span>, 2018</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The effect of utilizing superhydrophobic walls on improving the convective heat transfer in a rec...</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 effect of utilizing superhydrophobic walls on improving the convective heat transfer in a rectangular heatsink has been studied numerically in this paper. The vertical walls were kept at isothermal hot-and-cold temperatures and horizontal walls were insulated. The boundary condition on the walls was: no-slip for regular, and slip (with slip length of 500 µm) for superhydrophobic walls. By changing the heatsink aspect ratio (AR, height/width) from 0.1 to 10, it was observed that regardless of the wall slip, the optimum AR is 1, i.e. square enclosure. For a square heatsink, using the nanofluid with = 3% could enhance the heat transfer (quantified by Nusselt number) by up to 9.8%. For the same enclosure filled with pure water, applying superhydrophobic horizontal walls could increase the heat transfer by 4.45%. The joint effect of using superhydrophobic walls and nano-particles enhanced the heat transfer by up to 14.75%. The results of this paper may open a new avenue for high per...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="beadfe4d4a78fb3653b0937c66ff35de" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269274,"asset_id":72278832,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269274/download_file?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="72278832"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278832"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278832; 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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="72278831"><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/72278831/A_Diffusive_Model_for_Evaporation_of_Spherical_Water_Drops_at_Room_Temperature_and_Standard_Pressure"><img alt="Research paper thumbnail of A Diffusive Model for Evaporation of Spherical Water Drops at Room Temperature and Standard Pressure" class="work-thumbnail" src="https://attachments.academia-assets.com/81269270/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/72278831/A_Diffusive_Model_for_Evaporation_of_Spherical_Water_Drops_at_Room_Temperature_and_Standard_Pressure">A Diffusive Model for Evaporation of Spherical Water Drops at Room Temperature and Standard Pressure</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Evaporation of drops at room temperature and atmospheric conditions is mainly impelled by diffusi...</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">Evaporation of drops at room temperature and atmospheric conditions is mainly impelled by diffusion of vapor. Diffusion of vapor is a function of vapor concentration gradient (VCG) at the drop surface. The developed model in this paper modifies the relations used for finding the VCG for drops. The relations in literature for evaporation of millimetric drops are based on the study of Maxwell, which was originally for evaporation from a wet bulb. The VCG according to Maxwell based models is stationary and a function of the inverse of the bulb radius. However, where one uses this model for millimetric drops, the VCG becomes time dependent and increases in time (as during the evaporation, drop radius decreases). Intuitively it is understandable that the VCG should decrease in time (notwithstanding the Kelvin effect for very small microscopic drops). In this study a diffusion model is developed which uses a time dependent VCG that decreases in time. The developed diffusion model is able ...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="01d1712312456ab0d3563c7119be8d67" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269270,"asset_id":72278831,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269270/download_file?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="72278831"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278831"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278831; 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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="72278830"><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/72278830/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD_7003_Foil_A_Numerical_Approach"><img alt="Research paper thumbnail of Effect of Superhydrophobic Surface on Drag Coefficient of SD 7003 Foil : A Numerical Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/81269268/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/72278830/Effect_of_Superhydrophobic_Surface_on_Drag_Coefficient_of_SD_7003_Foil_A_Numerical_Approach">Effect of Superhydrophobic Surface on Drag Coefficient of SD 7003 Foil : A Numerical Approach</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">هلاقم تاعلاطا هدیکچ لهبک یطٍّظپ ِلبقه :تفبیسد 28 شْه 1395 :ششیزپ 21 سرآ 1395 :تیبس سد ِئاسا 91 يو...</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">هلاقم تاعلاطا هدیکچ لهبک یطٍّظپ ِلبقه :تفبیسد 28 شْه 1395 :ششیزپ 21 سرآ 1395 :تیبس سد ِئاسا 91 يوْث 9911 ِث یطشًا تلع یساَوّبً دَجٍ ٍ نک یحطس ةآ قَف حَطس یٍس شث لبیس ،ًَبً دبعثا سد بّ یه ضیشگ لَط صا شضغل يیا ىداد ىبطً یاشث .دضغل یه ُدبفتسا شیٍبً شضغل ًَبً ذٌچ دٍذح سد شضغل لَط یلَ وعه حَطس یاشث .دَض قَف حَطس یاشث یلٍ ،تسا شته یه ضیشگثآ بت ذًاَت μm 500 نّ اٍاشف تبعلبطه .ذسشث مبجًا بسپ یٍشیً شث ىآ شثا ٍ شضغل لَط یٍس شث یً ةآ قَف حطس لک ًلاَوعه تبعلبطه يیا سد .تسا ُذض یه ضیشگ .ددشگ شٍس ٌِیْث یحاَ ً يتفبی یاشث یه یدذع یبّ صیث یدذع تبعلبطه یلٍ ذضبث ذیفه ذًاَت یه تخت حَطس یٍس شث شت یٌحٌه حَطس یٍس شث .ذٌضبث لیَف ذًٌبه( یه ُذیچیپ ِلئسه یسسشث )صیاذج ىذهآ دَجٍ ِث ىبکها ٍ( یفٌه سبطف ىبیداشگ دَجٍ لیلد ِث )بّ ِث ِلبقه يیا سد .دَض یدذع تسَص لیَفٍسذیّ شضغل لَط شیثأت یسسشث ِث SD7003 صذلٌَیس سد تِخادشپ فلتخه یبّ .تسا ُذض نّ ٍ شیزپبً نکاشت ،ماسآ ىبیشج ِتفشگ شظً سد بهد شتٍ لَط بث مَیٌیهَلآ سٌج صا لیَفٍسذیّ ٍ ُذض cm 10 ةبختًا طشض ٍد سد بسپ تیشض ٍ سبطف تیشض ،یضشث صٌت تیشض جیبتً .تسا ُذض ُذض ِسیبقه شگیذکی...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="46ad7e7466129271220b8404c3840ed9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81269268,"asset_id":72278830,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81269268/download_file?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="72278830"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72278830"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72278830; 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