{"id":12981,"date":"2023-07-17T15:10:59","date_gmt":"2023-07-17T15:10:59","guid":{"rendered":"https:\/\/etc18.webs.upv.es\/?page_id=12981"},"modified":"2023-09-03T17:16:24","modified_gmt":"2023-09-03T17:16:24","slug":"monday-04","status":"publish","type":"page","link":"https:\/\/etc18.webs.upv.es\/index.php\/monday-04\/","title":{"rendered":"Monday 4th"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"12981\" class=\"elementor elementor-12981\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-8e3d2d7 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"67106\" data-id=\"8e3d2d7\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-a0d9984\" data-eae-slider=\"22134\" data-id=\"a0d9984\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-47d892a elementor-widget elementor-widget-heading\" data-id=\"47d892a\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">09:15 - 09:30 Meeting inauguration<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-d4b9c60 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"14530\" data-id=\"d4b9c60\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-b3eb235\" data-eae-slider=\"49160\" data-id=\"b3eb235\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-5b243cc elementor-widget elementor-widget-text-editor\" data-id=\"5b243cc\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/goo.gl\/maps\/oSAjfP1htyCMsazz6\"><b>NEXUS<\/b><\/a><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-0a4f502\" data-eae-slider=\"77146\" data-id=\"0a4f502\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-2d60058 elementor-widget elementor-widget-text-editor\" data-id=\"2d60058\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h3>Prof. Dr. Dolores Salvador, Deputy Chancellor for Employment and Lifelong Learning<\/h3>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-ec4b98c elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"3813\" data-id=\"ec4b98c\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-2ca8d1d\" data-eae-slider=\"97312\" data-id=\"2ca8d1d\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-d735c8e elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"d735c8e\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-9648514 elementor-widget elementor-widget-heading\" data-id=\"9648514\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">09:30 - 10:15 Keynote Speaker 1<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-41f4ed6 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"25922\" data-id=\"41f4ed6\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-7336430\" data-eae-slider=\"23828\" data-id=\"7336430\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-e5c6c47 elementor-widget elementor-widget-text-editor\" data-id=\"e5c6c47\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/goo.gl\/maps\/oSAjfP1htyCMsazz6\"><b>NEXUS<\/b><\/a><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-299d2ac\" data-eae-slider=\"16736\" data-id=\"299d2ac\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-dfa34a7 elementor-widget elementor-widget-text-editor\" data-id=\"dfa34a7\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h3><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/#leclainche\">Soledad Le Clainche<\/a><\/h3>\n<h4>Modal decompositions and other machine learning tools in fluid dynamics<\/h4>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-58430a4 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"88948\" data-id=\"58430a4\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-b74584c\" data-eae-slider=\"67374\" data-id=\"b74584c\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-e3a429d elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"e3a429d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-48c42c5 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"42693\" data-id=\"48c42c5\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-4abefb2\" data-eae-slider=\"13464\" data-id=\"4abefb2\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-404bba8 elementor-widget elementor-widget-heading\" data-id=\"404bba8\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">10:15 - 11:00 Keynote Speaker 2<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-45bffcd elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"42865\" data-id=\"45bffcd\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-4f2cefb\" data-eae-slider=\"26134\" data-id=\"4f2cefb\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-d2b2334 elementor-widget elementor-widget-text-editor\" data-id=\"d2b2334\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/goo.gl\/maps\/oSAjfP1htyCMsazz6\"><b>NEXUS<\/b><\/a><br><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-db2bc1e\" data-eae-slider=\"46389\" data-id=\"db2bc1e\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-72775af elementor-widget elementor-widget-text-editor\" data-id=\"72775af\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h3><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/#bagheri\">Shervin Bagheri<\/a><\/h3><h4>Functionality and stability of liquid-infused surfaces in shear flows<\/h4>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-edac5ee elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"44269\" data-id=\"edac5ee\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-3fce923\" data-eae-slider=\"82043\" data-id=\"3fce923\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-209a9ec elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"209a9ec\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-2948549 elementor-widget elementor-widget-heading\" data-id=\"2948549\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\"><a href=\"http:\/\/Functionality%20and%20stability%20of%20liquid-infused%20surfaces%20in%20shear%20flows\">11:00 - 11:30 Coffee Break <\/a><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-16f55cf elementor-widget elementor-widget-text-editor\" data-id=\"16f55cf\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h2 style=\"text-align: center;\"><a href=\"https:\/\/goo.gl\/maps\/77QsKryDQ6QmhwDCA\">ETSID<\/a><\/h2>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-ffc8e52 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"ffc8e52\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-54017f2 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"18344\" data-id=\"54017f2\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-472b0ac\" data-eae-slider=\"17025\" data-id=\"472b0ac\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-38e3823 elementor-widget elementor-widget-heading\" data-id=\"38e3823\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\"><a href=\"http:\/\/openmaps.upv.es\/?locate=V.7B.0.002\" target=\"_blank\">11:30 - 13:30 Parallel Session 1<\/a><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-6195731 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"51481\" data-id=\"6195731\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-12f717d\" data-eae-slider=\"30645\" data-id=\"12f717d\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-895be01 elementor-widget elementor-widget-accordion\" data-id=\"895be01\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"accordion.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1441\" class=\"elementor-tab-title\" data-tab=\"1\" role=\"button\" aria-controls=\"elementor-tab-content-1441\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Boundary Layers I, Sal\u00f3n de actos. Chair: Hasssan Nagib<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1441\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"1\" role=\"region\" aria-labelledby=\"elementor-tab-title-1441\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_12.pdf\" target=\"_blank\" rel=\"noopener\">12<\/a><\/td>\n<td class=\"tg-0lax\">Masoud Asadi, Pim Bullee and R.\u00a0 Jason Hearst<\/td>\n<td class=\"tg-0lax\">Streamwise evolution of the\u00a0\u00a0\u00a0interface between freestream turbulence and a turbulent boundary layer<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_24.pdf\">24<\/a><\/td>\n<td class=\"tg-0lax\">Marcos Piedrabuena, Ezhilsabareesh Kannadasan, Segio Hoyas, Ricardo Vinuesa and Hassan Nagib<\/td>\n<td class=\"tg-0lax\">Importance of Achieving Convergence for Computation of\u00a0\u00a0\u00a0Turbulence Through Pipes and Other Ducts<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_33.pdf\">33<\/a><\/td>\n<td class=\"tg-0lax\">Aron van den Bogaard, Ricardo Vinuesa, Ivan Marusic and Rahul\u00a0 Deshpande<\/td>\n<td class=\"tg-0lax\">Reynolds-number effects on the outer region of\u00a0\u00a0\u00a0adverse-pressure-gradient turbulent boundary layers<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_38.pdf\">38<\/a><\/td>\n<td class=\"tg-0lax\">Christopher Howland, Roberto Verzicco and Detlef Lohse<\/td>\n<td class=\"tg-0lax\">Non-monotonic heat flux in mixed vertical convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_100.pdf\">100<\/a><\/td>\n<td class=\"tg-0lax\">Esther M\u00e4teling, Wolfgang Schr\u00f6der and Christian Lagemann<\/td>\n<td class=\"tg-0lax\">High-accuracy turbulence statistics from particle images using\u00a0\u00a0\u00a0a deep optical flow neural network<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_130.pdf\">130<\/a><\/td>\n<td class=\"tg-0lax\">Vidya Vishwanathan, Ioannis Kaminaris, Ralph Volino, Elias\u00a0\u00a0\u00a0Balaras and Michael Schultz<\/td>\n<td class=\"tg-0lax\">Characteristics of Turbulent Boundary Layers Over\u00a0\u00a0\u00a0Heterogeneous Roughness<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_145.pdf\">145<\/a><\/td>\n<td class=\"tg-0lax\">Ke Zheng, Heri Setiawan, Kevin Kevin, Junghoon Lee and Jason\u00a0 Monty<\/td>\n<td class=\"tg-0lax\">Turbulent ship air-wake with ship motion<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_173.pdf\">173<\/a><\/td>\n<td class=\"tg-0lax\">Krishna Reddy Maryada, Steve Armfield, Priyanka Dhopade and\u00a0\u00a0\u00a0Stuart Norris<\/td>\n<td class=\"tg-0lax\">Self-similar energy-containing eddies in a turbulent natural\u00a0\u00a0\u00a0convection boundary layer immersed in a stably stratified medium<\/td>\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1442\" class=\"elementor-tab-title\" data-tab=\"2\" role=\"button\" aria-controls=\"elementor-tab-content-1442\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Atmospheric flows I. Room S01. Chair: Klara Jurcakova<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1442\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"2\" role=\"region\" aria-labelledby=\"elementor-tab-title-1442\"><table class=\"tg\"><tbody><tr><td class=\"tg-0lax\">11:30:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_34.pdf\" target=\"_blank\" rel=\"noopener\">34<\/a><\/td><td class=\"tg-0lax\">Florian Heyder, Juan Pedro Mellado and J\u00f6rg Schumacher<\/td><td class=\"tg-0lax\">Reservoir computing of a three-dimensional turbulent atmospheric boundary layer<\/td><\/tr><tr><td class=\"tg-0lax\">11:45:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_59.pdf\" target=\"_blank\" rel=\"noopener\">59<\/a><\/td><td class=\"tg-0lax\">Vladyslav Pushenko and J\u00f6rg Schumacher<\/td><td class=\"tg-0lax\">Turbulent mixing in the bulk of a cumulus cloud<\/td><\/tr><tr><td class=\"tg-0lax\">12:00:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_107.pdf\" target=\"_blank\" rel=\"noopener\">107<\/a><\/td><td class=\"tg-0lax\">Srikar V. Yadala, Girish K. Jankee, Leon Li, Nicholas A. Worth and R. Jason Hearst<\/td><td class=\"tg-0lax\">Impact of freestream turbulence on the recirculation region downstream of a backward-facing step<\/td><\/tr><tr><td class=\"tg-0lax\">12:15:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_131.pdf\" target=\"_blank\" rel=\"noopener\">131<\/a><\/td><td class=\"tg-0lax\">Kay Sch\u00e4fer, Juan Pedro Mellado and Bettina Frohnapfel<\/td><td class=\"tg-0lax\">The influence of spanwise heterogeneous surfaces on forced, mixed and natural convection<\/td><\/tr><tr><td class=\"tg-0lax\">12:30:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_180.pdf\" target=\"_blank\" rel=\"noopener\">180<\/a><\/td><td class=\"tg-0lax\">Babak Ranjbaran, Yuri Kanash, Ra\u00fal Bayo\u00e1n Cal and \u00c1rmann Gylfason<\/td><td class=\"tg-0lax\">An experimental study on the influence of gusts and suspended particles on the wake flow characteristics of wind turbines<\/td><\/tr><tr><td class=\"tg-0lax\">12:45:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_185.pdf\" target=\"_blank\" rel=\"noopener\">185<\/a><\/td><td class=\"tg-0lax\">Tomos Rich and Christina Vanderwel<\/td><td class=\"tg-0lax\">Turbulent Scalar Dispersion in the wake of an Individual Tall Building<\/td><\/tr><tr><td class=\"tg-0lax\">13:00:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_254.pdf\" target=\"_blank\" rel=\"noopener\">254<\/a><\/td><td class=\"tg-0lax\">Vamsi Krishna Chalamalla, Nitin Kumar and Anupam Dewan<\/td><td class=\"tg-0lax\">Large eddy simulations of forced plumes subjected to volumetric heating<\/td><\/tr><\/tbody><\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1443\" class=\"elementor-tab-title\" data-tab=\"3\" role=\"button\" aria-controls=\"elementor-tab-content-1443\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Geophysical flows I. Room S02. Chair: Jim Thomas<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1443\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"3\" role=\"region\" aria-labelledby=\"elementor-tab-title-1443\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_6.pdf\" target=\"_blank\" rel=\"noopener\">6<\/a><\/td>\n<td class=\"tg-0lax\">Jim Thomas<\/td>\n<td class=\"tg-0lax\">Upscale transfer of waves in one dimensional rotating shallow water<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_11.pdf\" target=\"_blank\" rel=\"noopener\">11<\/a><\/td>\n<td class=\"tg-0lax\">Sung Yong Kim<\/td>\n<td class=\"tg-0lax\">Geophysical turbulent characteristics of the remotely-sensed submesoscale surface currents and chlorophyll concentrations<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_18.pdf\" target=\"_blank\" rel=\"noopener\">18<\/a><\/td>\n<td class=\"tg-0lax\">Masanori Takaoka, Naoto Yokoyama and Eiichi Sasaki<\/td>\n<td class=\"tg-0lax\">Relation among zonal flow, Rossby radius, and triple cascade in two-dimensional equivalent barotropic vorticity turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_19.pdf\" target=\"_blank\" rel=\"noopener\">19<\/a><\/td>\n<td class=\"tg-0lax\">Shivam Swarnakar, Amitabh Bhattacharya and Sridhar Balasubramanian<\/td>\n<td class=\"tg-0lax\">Numerical investigation of rotating cylindrical annulus with bi-directional temperature gradients<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_43.pdf\" target=\"_blank\" rel=\"noopener\">43<\/a><\/td>\n<td class=\"tg-0lax\">Michele Buzzicotti, Benjamin Storer, Hemant Khatri, Stephen Griffies and Hussein Aluie<\/td>\n<td class=\"tg-0lax\">Energy Spectra and Cascades in the Global Ocean: Planetary Scales to Mesoscales, Surface to the Abyssal Ocean<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_63.pdf\" target=\"_blank\" rel=\"noopener\">63<\/a><\/td>\n<td class=\"tg-0lax\">Xiaojue Zhu, Olga Shishkina, Jiaxing Song and Shujaut Bader<\/td>\n<td class=\"tg-0lax\">On the diffusion-free regime in turbulent rapidly rotating convection and magnetoconvection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_82.pdf\" target=\"_blank\" rel=\"noopener\">82<\/a><\/td>\n<td class=\"tg-0lax\">Robert E. Ecke, Xuan Zhang and Olga Shishkina<\/td>\n<td class=\"tg-0lax\">The transition from wall modes to quasi-geostrophic rapidly rotating Rayleigh-Benard convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_96.pdf\" target=\"_blank\" rel=\"noopener\">96<\/a><\/td>\n<td class=\"tg-0lax\">Vinay Tripathi and Pranav Joshi<\/td>\n<td class=\"tg-0lax\">Phenomenon of Ekman pumping in rotating Rayleigh-Be \u0301nard convection with boundary roughness<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1444\" class=\"elementor-tab-title\" data-tab=\"4\" role=\"button\" aria-controls=\"elementor-tab-content-1444\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Multiphase and Non-Newtonian I, Room S03. Chair: Cristian Marchioli<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1444\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"4\" role=\"region\" aria-labelledby=\"elementor-tab-title-1444\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_28.pdf\" target=\"_blank\" rel=\"noopener\">28<\/a><\/td>\n<td class=\"tg-0lax\">Julien Carlier and Miltiadis Papalexandris<\/td>\n<td class=\"tg-0lax\">Numerical study of natural convection of an air-water system with evaporation across the free surface<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_36.pdf\" target=\"_blank\" rel=\"noopener\">36<\/a><\/td>\n<td class=\"tg-0lax\">Ingu Lee, Jaehee Chang and Haecheon Choi<\/td>\n<td class=\"tg-0lax\">Numerical study on a turbulent bubbly pipe flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_50.pdf\" target=\"_blank\" rel=\"noopener\">50<\/a><\/td>\n<td class=\"tg-0lax\">Cristian Marchioli and Davide Di Giusto<\/td>\n<td class=\"tg-0lax\">Flexible fibers in turbulent channel flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_64.pdf\" target=\"_blank\" rel=\"noopener\">64<\/a><\/td>\n<td class=\"tg-0lax\">Leonardo Puggioni, Guido Boffetta and Stefano Musacchio<\/td>\n<td class=\"tg-0lax\">Flocking turbulence of microswimmers in confined domains<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_66.pdf\" target=\"_blank\" rel=\"noopener\">66<\/a><\/td>\n<td class=\"tg-0lax\">Stefano Musacchio, Leonardo Puggioni and Guido Boffetta<\/td>\n<td class=\"tg-0lax\">Giant vortex dynamics in confined bacterial turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_69.pdf\" target=\"_blank\" rel=\"noopener\">69<\/a><\/td>\n<td class=\"tg-0lax\">Himani Garg, Christer Fureby and Lei Wang<\/td>\n<td class=\"tg-0lax\">Polymer-induced turbulence in 2D micro-serpentine channel<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_83.pdf\" target=\"_blank\" rel=\"noopener\">83<\/a><\/td>\n<td class=\"tg-0lax\">Zhiwen Cui, Jingran Qiu, Xinyu Jiang and Lihao Zhao<\/td>\n<td class=\"tg-0lax\">Effect of fluid-inertial torque on the orientation of tiny spheroidal particles in turbulent channel flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_85.pdf\" target=\"_blank\" rel=\"noopener\">85<\/a><\/td>\n<td class=\"tg-0lax\">Chao Sun, Yihong Du, Ziqi Wang, Linfeng Jiang and Enrico Calzavarini<\/td>\n<td class=\"tg-0lax\">Sea Water Freezing Modes in a Natural Convection System<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1445\" class=\"elementor-tab-title\" data-tab=\"5\" role=\"button\" aria-controls=\"elementor-tab-content-1445\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Control of Turbulent flows I. Room S04. Chair: Maurizio Quadrio<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1445\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"5\" role=\"region\" aria-labelledby=\"elementor-tab-title-1445\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_25.pdf\" target=\"_blank\" rel=\"noopener\">25<\/a><\/td>\n<td class=\"tg-0lax\">Mohammad Umair and Sedat Tardu<\/td>\n<td class=\"tg-0lax\">Turbulent channel flow under large amplitude streamwise travelling waves<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_67.pdf\" target=\"_blank\" rel=\"noopener\">67<\/a><\/td>\n<td class=\"tg-0lax\">Arvind Mohan, Surya Chakrabarti, Datta Gaitonde and Daniel Livescu<\/td>\n<td class=\"tg-0lax\">Full trajectory optimizing operator inference for reduced-order modeling using differentiable programming<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_106.pdf\" target=\"_blank\" rel=\"noopener\">106<\/a><\/td>\n<td class=\"tg-0lax\">Giacomo Della Posta, Emanuele Martelli, Francesco Salvadore and Matteo Bernardini<\/td>\n<td class=\"tg-0lax\">Direct Numerical Simulation of Microramp Vortex Generators for Shock Wave\/Boundary Layer Interaction Control<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_125.pdf\" target=\"_blank\" rel=\"noopener\">125<\/a><\/td>\n<td class=\"tg-0lax\">Emanuele Gallorini and Maurizio Quadrio<\/td>\n<td class=\"tg-0lax\">Effect of control discretization on streamwise traveling waves of spanwise wall velocity<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_126.pdf\" target=\"_blank\" rel=\"noopener\">126<\/a><\/td>\n<td class=\"tg-0lax\">Alessandro Scala, Carlo Salvatore Greco, Gerardo Paolillo, Tommaso Astarita and Gennaro Cardone<\/td>\n<td class=\"tg-0lax\">Influence of Machine Learning-based active flow control on the turbulent statistics of the flow over a circular cylinder<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_132.pdf\" target=\"_blank\" rel=\"noopener\">132<\/a><\/td>\n<td class=\"tg-0lax\">Amirreza Rouhi, Matt Fu, Dileep Chandran, Andrea Zampiron, Alexander Smits and Ivan Marusic<\/td>\n<td class=\"tg-0lax\">Large-eddy simulations of turbulent drag reduction by spanwise wall forcing up to Re_tau = 4000<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_137.pdf\" target=\"_blank\" rel=\"noopener\">137<\/a><\/td>\n<td class=\"tg-0lax\">Weiqi Sun, Jimmy Philip, Wolfgang Schroeder and Joseph Klewicki<\/td>\n<td class=\"tg-0lax\">A comparative study of artificial and natural streamwise vortices in the near-wall region of turbulent boundary layers<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_169.pdf\" target=\"_blank\" rel=\"noopener\">169<\/a><\/td>\n<td class=\"tg-0lax\">Rahul Deshpande, Aman G. Kidanemariam and Ivan Marusic<\/td>\n<td class=\"tg-0lax\">Pressure drag reduction via imposition of spanwise wall oscillations on a rod-roughened wall<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1446\" class=\"elementor-tab-title\" data-tab=\"6\" role=\"button\" aria-controls=\"elementor-tab-content-1446\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Vortex Dynamics I. Room S05. Chair: Gerrit Elsinga<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1446\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"6\" role=\"region\" aria-labelledby=\"elementor-tab-title-1446\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_1.pdf\" target=\"_blank\" rel=\"noopener\">1<\/a><\/td>\n<td class=\"tg-0lax\">Ondrej Fercak, Zein Sadek, Trevor Dunt, Christin Murphy, Jennifer Franck and Ra\u00fal Bayo\u00e1n Cal<\/td>\n<td class=\"tg-0lax\">Flow Structure Dynamics in Arrays of Undulated Cylinders<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_7.pdf\" target=\"_blank\" rel=\"noopener\">7<\/a><\/td>\n<td class=\"tg-0lax\">Ping-Fan Yang, Zhideng Zhou, Jian Fang, Le Fang, Haitao Xu, Guowei He and Alain Pumir<\/td>\n<td class=\"tg-0lax\">Generalized Betchov relations for vector fields and their applications in turbulent flows<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_8.pdf\" target=\"_blank\" rel=\"noopener\">8<\/a><\/td>\n<td class=\"tg-0lax\">Mahendra Verma and Soumyadeep Chatterjee<\/td>\n<td class=\"tg-0lax\">Emergence of Order in 2D Euler Turbulence, an Isolated System<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_42.pdf\" target=\"_blank\" rel=\"noopener\">42<\/a><\/td>\n<td class=\"tg-0lax\">Masahiro Suzuki and Nobuyuki Okura<\/td>\n<td class=\"tg-0lax\">Flow instability under an elongated plate above the ground<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_46.pdf\" target=\"_blank\" rel=\"noopener\">46<\/a><\/td>\n<td class=\"tg-0lax\">Anton Svirsky, Corentin Herbert and Anna Frishman<\/td>\n<td class=\"tg-0lax\">Two-dimensional turbulence with local interactions: statistics of the condensate<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_60.pdf\" target=\"_blank\" rel=\"noopener\">60<\/a><\/td>\n<td class=\"tg-0lax\">Veeraraghavan Kannan and Xiaojue Zhu<\/td>\n<td class=\"tg-0lax\">Turbulent Rapidly Rotating Rayleigh-Benard Convection: Cyclones Vs Anti-Cyclones<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_72.pdf\" target=\"_blank\" rel=\"noopener\">72<\/a><\/td>\n<td class=\"tg-0lax\">Bernard Geurts, Liesbeth Klein Kranenbarg, Stijn Peereboom and Rudie Kunnen<\/td>\n<td class=\"tg-0lax\">Nusselt-Rossby scaling in high-frequency harmonic modulation of rotating Rayleigh-Benard convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_75.pdf\" target=\"_blank\" rel=\"noopener\">75<\/a><\/td>\n<td class=\"tg-0lax\">Tong Wu and Wouter Bos<\/td>\n<td class=\"tg-0lax\">Point-vortex statistical mechanics applied to turbulence without vortex stretching<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1447\" class=\"elementor-tab-title\" data-tab=\"7\" role=\"button\" aria-controls=\"elementor-tab-content-1447\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Geophysical Flows II. Room S06. Chair: Louis Couston<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1447\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"7\" role=\"region\" aria-labelledby=\"elementor-tab-title-1447\"><table class=\"tg\"><tbody><tr><td class=\"tg-0lax\">11:30:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_428.pdf\" target=\"_blank\" rel=\"noopener\">428<\/a><\/td><td class=\"tg-0lax\">Olav R\u00f8mcke, Benjamin K. Smeltzer, Inger Skundberg L\u00f8vvig, Johannes Djupesland, R. Jason Hearst and Simen \u00c5. Ellingsen<\/td><td class=\"tg-0lax\">Experiment on turbulence developing under surface waves<\/td><\/tr><tr><td class=\"tg-0lax\">11:45:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_434.pdf\" target=\"_blank\" rel=\"noopener\">434<\/a><\/td><td class=\"tg-0lax\">Paul Mannix, David Ham and John Craske<\/td><td class=\"tg-0lax\">The probability density behind thermal stratifications sustained by uncertain and heterogeneous forcing<\/td><\/tr><tr><td class=\"tg-0lax\">12:00:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_448.pdf\" target=\"_blank\" rel=\"noopener\">448<\/a><\/td><td class=\"tg-0lax\">Catherine Vreugdenhil, Nicholas Wilson, Bishakhdatta Gayen and Eric Hester<\/td><td class=\"tg-0lax\">The effects of ocean turbulence and double-diffusive layering on the melting of ice shelves<\/td><\/tr><tr><td class=\"tg-0lax\">12:15:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_465.pdf\" target=\"_blank\" rel=\"noopener\">465<\/a><\/td><td class=\"tg-0lax\">Victor Avsarkisov, Niklas Dusch, Michael Gerding, Jens S\u00f6der and Claudia Stolle<\/td><td class=\"tg-0lax\">Kinetic Helicity in the Turbulent Stratified Flows<\/td><\/tr><tr><td class=\"tg-0lax\">12:30:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_482.pdf\" target=\"_blank\" rel=\"noopener\">482<\/a><\/td><td class=\"tg-0lax\">Georges Edde, Georges Sadaka, Rapha\u00ebl Antoine and Ionut Danaila<\/td><td class=\"tg-0lax\">Numerical modeling of air flows in an underground cavity connected to the surface by a shaft<\/td><\/tr><tr><td class=\"tg-0lax\">12:45:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_429.pdf\" target=\"_blank\" rel=\"noopener\">429<\/a><\/td><td class=\"tg-0lax\">Petr Michalek, Stanislav Pospisil and Pavel Sedlak<\/td><td class=\"tg-0lax\">Study of atmospheric turbulence characteristics in Northwest Bohemia<\/td><\/tr><tr><td class=\"tg-0lax\">13:00:00<\/td><td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_489.pdf\" target=\"_blank\" rel=\"noopener\">489<\/a><\/td><td class=\"tg-0lax\">Sara Mata, Bruno Scapin and Jorge Silvestrini<\/td><td class=\"tg-0lax\">Turbulence in particle-laden gravity currents trough iLES<\/td><\/tr><\/tbody><\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1448\" class=\"elementor-tab-title\" data-tab=\"8\" role=\"button\" aria-controls=\"elementor-tab-content-1448\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Transport and Mixing I. Room N01. Chair: Geert Brethouwer<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1448\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"8\" role=\"region\" aria-labelledby=\"elementor-tab-title-1448\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_21.pdf\" target=\"_blank\" rel=\"noopener\">21<\/a><\/td>\n<td class=\"tg-0lax\">Ke-Qing Xia, Yun-Bing Hu and Lin Sun<\/td>\n<td class=\"tg-0lax\">On the Effect of Centrifugal Force in Turbulent Thermal Convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_35.pdf\" target=\"_blank\" rel=\"noopener\">35<\/a><\/td>\n<td class=\"tg-0lax\">David Rodr\u00edguez-Guti\u00e9rrez, Andrea Gruber, Raquel G\u00f3mez-Miguel, Mario S\u00e1nchez-Sanz and Eduardo Fern\u00e1ndez-Tarrazo<\/td>\n<td class=\"tg-0lax\">Numerical study of H2-air turbulent mixing processes using a selective permeable injection technique<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_51.pdf\" target=\"_blank\" rel=\"noopener\">51<\/a><\/td>\n<td class=\"tg-0lax\">Khashayar Feizbakhshian Kohan and Susan Gaskin<\/td>\n<td class=\"tg-0lax\">Effect of background turbulence on the scalar entrainment into a jet: width of the scalar interface and evidence of detrainment<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_93.pdf\" target=\"_blank\" rel=\"noopener\">93<\/a><\/td>\n<td class=\"tg-0lax\">Jiangang Chen and Oliver Buxton<\/td>\n<td class=\"tg-0lax\">Spatial evolution of the turbulent\/turbulent interface geometry and turbulent momentum entrainment<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_103.pdf\" target=\"_blank\" rel=\"noopener\">103<\/a><\/td>\n<td class=\"tg-0lax\">Lu Zhang, Jing Dong and Ke-Qing Xia<\/td>\n<td class=\"tg-0lax\">The interplay between horizontal heat transfer and large scale circulation in turbulent Rayleigh-Benard convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_121.pdf\" target=\"_blank\" rel=\"noopener\">121<\/a><\/td>\n<td class=\"tg-0lax\">Ingrid Neunaber, Masoud Asadi, Leon Li and R. Jason Hearst<\/td>\n<td class=\"tg-0lax\">Turbulence fields generated by a flapping active grid: Comparing hot-wire and particle image velocimetry<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_199.pdf\" target=\"_blank\" rel=\"noopener\">199<\/a><\/td>\n<td class=\"tg-0lax\">Geert Brethouwer<\/td>\n<td class=\"tg-0lax\">The effect of rotation on heat and momentum transport and structures in plane Couette and Taylor-Couette flow<\/td>\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1449\" class=\"elementor-tab-title\" data-tab=\"9\" role=\"button\" aria-controls=\"elementor-tab-content-1449\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Instability and Transition I. Room AirNostrum. Chair: Marc Avila <\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1449\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"9\" role=\"region\" aria-labelledby=\"elementor-tab-title-1449\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">11:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_4.pdf\" target=\"_blank\" rel=\"noopener\">4<\/a><\/td>\n<td class=\"tg-0lax\">Zhongyu Zhang and Xuesong Wu<\/td>\n<td class=\"tg-0lax\">Unified dynamic and aeroacoustic theories for the ring-mode coherent structures in all flow regions of a subsonic turbulent jet<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">11:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_14.pdf\" target=\"_blank\" rel=\"noopener\">14<\/a><\/td>\n<td class=\"tg-0lax\">Ming Dong and Runjie Song<\/td>\n<td class=\"tg-0lax\">Linear and nonlinear instability of supersonic boundary layers over a rotating cone<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_15.pdf\" target=\"_blank\" rel=\"noopener\">15<\/a><\/td>\n<td class=\"tg-0lax\">Ewa Tuliszka-Sznitko<\/td>\n<td class=\"tg-0lax\">The flow regimes in the short Taylor-Couette configurations with independently rotating cylinders, aspect ratio 0.5<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_31.pdf\" target=\"_blank\" rel=\"noopener\">31<\/a><\/td>\n<td class=\"tg-0lax\">Ivan Kharsansky Atallah, Luc Pastur, Romain Monchaux and Laurent Zimmer<\/td>\n<td class=\"tg-0lax\">From Low-Frequency Oscillations to Markovian Bistable Stall Dynamics<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_41.pdf\" target=\"_blank\" rel=\"noopener\">41<\/a><\/td>\n<td class=\"tg-0lax\">Guang-Yu Ding and Ke-Qing Xia<\/td>\n<td class=\"tg-0lax\">Heat transport and flow morphology of geostrophic rotating Rayleigh-B\u00e9nard convection in the presence of boundary flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">12:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_45.pdf\" target=\"_blank\" rel=\"noopener\">45<\/a><\/td>\n<td class=\"tg-0lax\">Till Zeugin, Daniel Mor\u00f3n, Marc Avila and Markus Holzner<\/td>\n<td class=\"tg-0lax\">Transition to turbulence of pulsatile flow in flexible pipes<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_52.pdf\" target=\"_blank\" rel=\"noopener\">52<\/a><\/td>\n<td class=\"tg-0lax\">Daeun Song and Haecheon Choi<\/td>\n<td class=\"tg-0lax\">Characteristics of turbulent flow past a vertical flat plate<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">13:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_55.pdf\" target=\"_blank\" rel=\"noopener\">55<\/a><\/td>\n<td class=\"tg-0lax\">Haoyan Wu and Baofang Song<\/td>\n<td class=\"tg-0lax\">The Re-scaling of the propagation speed of turbulent fronts in pipe flow<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-38d97d7 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"18418\" data-id=\"38d97d7\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-c7c822c\" data-eae-slider=\"76637\" data-id=\"c7c822c\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-2d643ba elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"2d643ba\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-7d491b2 elementor-widget elementor-widget-heading\" data-id=\"7d491b2\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\"><a href=\"http:\/\/Functionality%20and%20stability%20of%20liquid-infused%20surfaces%20in%20shear%20flows\">13:30 - 15:00 Giant Paella! <\/a><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-a6f867e elementor-widget elementor-widget-text-editor\" data-id=\"a6f867e\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h1 style=\"text-align: center;\">Check location!<\/h1>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-6eeb096 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"6eeb096\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-c7a5c0f elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"19967\" data-id=\"c7a5c0f\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-c795f7d\" data-eae-slider=\"13296\" data-id=\"c795f7d\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-c870f79 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"c870f79\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-b08e797 elementor-widget elementor-widget-heading\" data-id=\"b08e797\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">15:00 - 15:45 Keynote Speaker 3<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-11d5091 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"374\" data-id=\"11d5091\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-0387ba2\" data-eae-slider=\"7532\" data-id=\"0387ba2\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-ffb549d elementor-widget elementor-widget-text-editor\" data-id=\"ffb549d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/goo.gl\/maps\/oSAjfP1htyCMsazz6\"><b>NEXUS<\/b><\/a><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-1fcee7c\" data-eae-slider=\"7126\" data-id=\"1fcee7c\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-a6b4528 elementor-widget elementor-widget-text-editor\" data-id=\"a6b4528\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h3><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/#salvetti\">Mar\u00eda Vittoria Salvetti<\/a><\/h3><h4 style=\"font-size: 16px; text-align: justify;\">Dynamics of separating and reattaching flows<\/h4>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-67a69da elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"14778\" data-id=\"67a69da\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-3c6fa2c\" data-eae-slider=\"59313\" data-id=\"3c6fa2c\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-e33ad97 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"e33ad97\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-76d0d75 elementor-widget elementor-widget-heading\" data-id=\"76d0d75\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">15:45 - 16:30 Keynote Speaker 4<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-f9d13a5 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"75058\" data-id=\"f9d13a5\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-db21a7e\" data-eae-slider=\"57956\" data-id=\"db21a7e\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-db81aff elementor-widget elementor-widget-text-editor\" data-id=\"db81aff\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/goo.gl\/maps\/oSAjfP1htyCMsazz6\"><b>NEXUS<\/b><\/a><br><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-985f373\" data-eae-slider=\"32650\" data-id=\"985f373\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-deadc13 elementor-widget elementor-widget-text-editor\" data-id=\"deadc13\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h3><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/#vinuesa\">Ricardo Vinuesa<\/a><\/h3><h4 style=\"font-size: 16px; text-align: justify;\">Modeling and controlling turbulent flows through deep learning<\/h4>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-1e5000e elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"89735\" data-id=\"1e5000e\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-087b7a9\" data-eae-slider=\"17695\" data-id=\"087b7a9\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-e9f635f elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"e9f635f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-b680d0a elementor-widget elementor-widget-heading\" data-id=\"b680d0a\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\"><a href=\"http:\/\/Functionality%20and%20stability%20of%20liquid-infused%20surfaces%20in%20shear%20flows\">16:30 - 17:00 Coffee Break <\/a><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-0e9b8aa elementor-widget elementor-widget-text-editor\" data-id=\"0e9b8aa\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h2 style=\"text-align: center;\"><a href=\"https:\/\/goo.gl\/maps\/77QsKryDQ6QmhwDCA\">ETSID<\/a><\/h2>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-c23f58f elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"c23f58f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"divider.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-divider\">\n\t\t\t<span class=\"elementor-divider-separator\">\n\t\t\t\t\t\t<\/span>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-eff7398 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"23194\" data-id=\"eff7398\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-186a73d\" data-eae-slider=\"79468\" data-id=\"186a73d\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-519b37d elementor-widget elementor-widget-heading\" data-id=\"519b37d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\"><a href=\"http:\/\/openmaps.upv.es\/?locate=V.7B.0.002\" target=\"_blank\">17:00 - 19:00 Parallel Session 2<\/a><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-b8836f7 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"83952\" data-id=\"b8836f7\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-c203d18\" data-eae-slider=\"13709\" data-id=\"c203d18\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-c9687ec elementor-widget elementor-widget-accordion\" data-id=\"c9687ec\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"accordion.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2111\" class=\"elementor-tab-title\" data-tab=\"1\" role=\"button\" aria-controls=\"elementor-tab-content-2111\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Wall-Bounded Flows - Theory I. Room Salon de actos. Chair: Julio Soria<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2111\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"1\" role=\"region\" aria-labelledby=\"elementor-tab-title-2111\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_26.pdf\" target=\"_blank\" rel=\"noopener\">26<\/a><\/td>\n<td class=\"tg-0lax\">Nicola Ciola, Pietro De Palma, Jean-Christophe Robinet and Stefania Cherubini<\/td>\n<td class=\"tg-0lax\">A local mechanism linked to the emergence of extreme events in the turbulent channel flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_30.pdf\" target=\"_blank\" rel=\"noopener\">30<\/a><\/td>\n<td class=\"tg-0lax\">Javier Jimenez<\/td>\n<td class=\"tg-0lax\">Perron-Frobenius analysis of bursting in wall turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_113.pdf\" target=\"_blank\" rel=\"noopener\">113<\/a><\/td>\n<td class=\"tg-0lax\">Guowei He and Ting Wu<\/td>\n<td class=\"tg-0lax\">Composition of resolvents enhanced by random sweeping for large-scale structures in turbulent channel flows<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_140.pdf\" target=\"_blank\" rel=\"noopener\">140<\/a><\/td>\n<td class=\"tg-0lax\">Ezhilsabareesh Kannadasan, Callum Atkinson and Julio Soria<\/td>\n<td class=\"tg-0lax\">Interscale transport mechanisms in the spatial evolution of energy-containing eddies<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_142.pdf\" target=\"_blank\" rel=\"noopener\">142<\/a><\/td>\n<td class=\"tg-0lax\">Luka Lindic, Rahul Deshpande and Ivan Marusic<\/td>\n<td class=\"tg-0lax\">Canonical inflow adverse pressure gradient turbulent boundary layers at high Reynolds number<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_158.pdf\" target=\"_blank\" rel=\"noopener\">158<\/a><\/td>\n<td class=\"tg-0lax\">Mariangela De Maio, Beatrice Latini, Francesco Nasuti and Sergio Pirozzoli<\/td>\n<td class=\"tg-0lax\">Heat and mass transfer of flow inside pipes with large relative roughness height<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_168.pdf\" target=\"_blank\" rel=\"noopener\">168<\/a><\/td>\n<td class=\"tg-0lax\">Daniel Mor\u00f3n Montesdeoca, Alberto Vela-Mart\u00edn and Marc Avila<\/td>\n<td class=\"tg-0lax\">Predictability of puff decay in pipe flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_408.pdf\" target=\"_blank\" rel=\"noopener\">408<\/a><\/td>\n<td class=\"tg-0lax\">T.-W. Lee and J.E. Park<\/td>\n<td class=\"tg-0lax\">A Dynamical Transport Theory of Wall-Bounded Turbulent Flows<\/td>\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2112\" class=\"elementor-tab-title\" data-tab=\"2\" role=\"button\" aria-controls=\"elementor-tab-content-2112\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Boundary Layers II. Room S01. Chair: Sergio Hoyas<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2112\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"2\" role=\"region\" aria-labelledby=\"elementor-tab-title-2112\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_182.pdf\" target=\"_blank\" rel=\"noopener\">182<\/a><\/td>\n<td class=\"tg-0lax\">Jason Appelbaum and Christoph Wenzel<\/td>\n<td class=\"tg-0lax\">Influence of Streamline Curvature on Compressible Turbulent Boundary Layers<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_189.pdf\" target=\"_blank\" rel=\"noopener\">189<\/a><\/td>\n<td class=\"tg-0lax\">Jia-Qi Ma, Sheng-Hong Peng, Wen-Feng Li and Heng-Dong Xi<\/td>\n<td class=\"tg-0lax\">Modifications of the friction drag and coherent structures in turbulent boundary layers via local polymer solution ejection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_222.pdf\" target=\"_blank\" rel=\"noopener\">222<\/a><\/td>\n<td class=\"tg-0lax\">Joseph Barrow, Tao Liu, Michael Wilkes, Barry Gallacher and Richard Whalley<\/td>\n<td class=\"tg-0lax\">On the development of an optical MEMS sensor for instantaneous wall-shear stress measurements in wall-bounded turbulent flows<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_240.pdf\" target=\"_blank\" rel=\"noopener\">240<\/a><\/td>\n<td class=\"tg-0lax\">Pei-Yun Tsai, Heiko Schmidt and Marten Klein<\/td>\n<td class=\"tg-0lax\">Stochastic modeling of heated turbulent coaxial pipe flow prescribing different thermal boundary conditions<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_244.pdf\" target=\"_blank\" rel=\"noopener\">244<\/a><\/td>\n<td class=\"tg-0lax\">Marie Ono, Noriyuki Furuichi and Yoshiyuki Tsuji<\/td>\n<td class=\"tg-0lax\">Scaling of turbulence statistics for three velocity components and turbulence kinetic energy in pipe flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_301.pdf\" target=\"_blank\" rel=\"noopener\">301<\/a><\/td>\n<td class=\"tg-0lax\">Miaoyan Pang and Kapil Chauhan<\/td>\n<td class=\"tg-0lax\">Self-similarity of moments of concentration fluctuations in a plume<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_316.pdf\" target=\"_blank\" rel=\"noopener\">316<\/a><\/td>\n<td class=\"tg-0lax\">Keshanjali Gaur<\/td>\n<td class=\"tg-0lax\">Nano-scale sensors for wall-shear-stress measurements<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_334.pdf\" target=\"_blank\" rel=\"noopener\">334<\/a><\/td>\n<td class=\"tg-0lax\">Fahrettin G\u00f6khan Ergin, Frederik Zafiryadis, Bo Watz and Knud Erik Meyer<\/td>\n<td class=\"tg-0lax\">A spatial-resolution correction scheme for disturbance profiles in a developing zero-pressure-gradient turbulent boundary layer<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2113\" class=\"elementor-tab-title\" data-tab=\"3\" role=\"button\" aria-controls=\"elementor-tab-content-2113\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Geophysical Flows III. Room S02. Chair: Berengere\tDubrulle<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2113\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"3\" role=\"region\" aria-labelledby=\"elementor-tab-title-2113\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_146.pdf\" target=\"_blank\" rel=\"noopener\">146<\/a><\/td>\n<td class=\"tg-0lax\">Avishek Ranjan and Peter Davidson<\/td>\n<td class=\"tg-0lax\">Turbulent diffusion of heat near the equator and its connection with helicity segregation in geodynamo simulations<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_175.pdf\" target=\"_blank\" rel=\"noopener\">175<\/a><\/td>\n<td class=\"tg-0lax\">Julie Meunier, Basile Gallet and Benjamin Miquel<\/td>\n<td class=\"tg-0lax\">Three-dimensional structure of transport by ocean mesoscale turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_176.pdf\" target=\"_blank\" rel=\"noopener\">176<\/a><\/td>\n<td class=\"tg-0lax\">Gabriel Hadjerci, Vincent Bouillaut, Benjamin Miquel, S\u00e9bastien Auma\u00eetre and Basile Gallet<\/td>\n<td class=\"tg-0lax\">Ultimate regime of rapidly rotating convection: experimental and numerical assessment of the `geostrophic turbulence&#8217; scaling predictions<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_287.pdf\" target=\"_blank\" rel=\"noopener\">287<\/a><\/td>\n<td class=\"tg-0lax\">Basile Gallet, Vincent Bouillaut, Gabriel Hadjerci, Benjamin Miquel, Keith Julien and S\u00e9bastien Auma\u00eetre<\/td>\n<td class=\"tg-0lax\">Experimental observation of the geostrophic turbulence regime of rapidly rotating convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_364.pdf\" target=\"_blank\" rel=\"noopener\">364<\/a><\/td>\n<td class=\"tg-0lax\">Lucas Fery, B\u00e9reng\u00e8re Dubrulle, B\u00e9reng\u00e8re Podvin, Flavio Pons and Davide Faranda<\/td>\n<td class=\"tg-0lax\">Decomposing weather maps into interpretable patterns using Latent Dirichlet Allocation<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_371.pdf\" target=\"_blank\" rel=\"noopener\">371<\/a><\/td>\n<td class=\"tg-0lax\">Jean-Cl\u00e9ment Ringenbach, Tobias Schneider and Steven Tobias<\/td>\n<td class=\"tg-0lax\">Heat transport in rotating convection captured by invariant solutions<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_417.pdf\" target=\"_blank\" rel=\"noopener\">417<\/a><\/td>\n<td class=\"tg-0lax\">Alban Potherat, Rishav Agrawal and Aujogue Kelig<\/td>\n<td class=\"tg-0lax\">Quasi-two dimensionality and the Magnetic Taylor-Proudman constraint in rotating magneto-convection<\/td>\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2114\" class=\"elementor-tab-title\" data-tab=\"4\" role=\"button\" aria-controls=\"elementor-tab-content-2114\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Multiphase and  Non-Newtonian II. Room S03. Chair: Filippo\tColetti<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2114\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"4\" role=\"region\" aria-labelledby=\"elementor-tab-title-2114\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_91.pdf\" target=\"_blank\" rel=\"noopener\">91<\/a><\/td>\n<td class=\"tg-0lax\">Marco Edoardo Rosti, Prasad Perlekar and Dhrubaditya Mitra<\/td>\n<td class=\"tg-0lax\">Elastic range scaling in polymeric turbulence at large Reynolds and Deborah numbers<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_94.pdf\" target=\"_blank\" rel=\"noopener\">94<\/a><\/td>\n<td class=\"tg-0lax\">Simone Tandurella, Guido Boffetta, Stefano Musacchio and Marco E. Rosti<\/td>\n<td class=\"tg-0lax\">Inertial particles Rayleigh-Taylor turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_98.pdf\" target=\"_blank\" rel=\"noopener\">98<\/a><\/td>\n<td class=\"tg-0lax\">Alessandro Chiarini, Ianto Cannon and Marco E. Rosti<\/td>\n<td class=\"tg-0lax\">Turbulence modulation by finite-size spherical particles<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_101.pdf\" target=\"_blank\" rel=\"noopener\">101<\/a><\/td>\n<td class=\"tg-0lax\">Daniel Ruth and Filippo Coletti<\/td>\n<td class=\"tg-0lax\">Scale-to-scale energy transfer in the turbulence near a free surface<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_110.pdf\" target=\"_blank\" rel=\"noopener\">110<\/a><\/td>\n<td class=\"tg-0lax\">Wei Gao, Matteo Parsani and Pedro Costa<\/td>\n<td class=\"tg-0lax\">Particle-resolved simulations of positively-buoyant particles in the open channel flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_111.pdf\" target=\"_blank\" rel=\"noopener\">111<\/a><\/td>\n<td class=\"tg-0lax\">Alessandro Capone, Giorgio Moscato and Giovanni Paolo Romano<\/td>\n<td class=\"tg-0lax\">Solid Particle Dispersion in a Turbulent Jet<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_112.pdf\" target=\"_blank\" rel=\"noopener\">112<\/a><\/td>\n<td class=\"tg-0lax\">Aswathy M S and Marco E Rosti<\/td>\n<td class=\"tg-0lax\">Dynamics of flexible fibres immersed in viscoelastic fluids<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_117.pdf\" target=\"_blank\" rel=\"noopener\">117<\/a><\/td>\n<td class=\"tg-0lax\">St\u00e9phane Fischer and Marie Burckbuchler<\/td>\n<td class=\"tg-0lax\">Sediment transport measurements with a multi-component ultrasonic profiler<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2115\" class=\"elementor-tab-title\" data-tab=\"5\" role=\"button\" aria-controls=\"elementor-tab-content-2115\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Control of Turbulent flows II. Room S04. Chair: Ian Jacobi<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2115\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"5\" role=\"region\" aria-labelledby=\"elementor-tab-title-2115\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_171.pdf\" target=\"_blank\" rel=\"noopener\">171<\/a><\/td>\n<td class=\"tg-0lax\">Sina Nozarian, Mahdi Abkar and Pourya Forooghi<\/td>\n<td class=\"tg-0lax\">A study of drag reduction on rough walls using spanwise opposed wall-jet forcing<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_184.pdf\" target=\"_blank\" rel=\"noopener\">184<\/a><\/td>\n<td class=\"tg-0lax\">Pawe\u0142 Baj<\/td>\n<td class=\"tg-0lax\">Large-scale motion in a baffled von K\u00e1rm\u00e1n tank<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_192.pdf\" target=\"_blank\" rel=\"noopener\">192<\/a><\/td>\n<td class=\"tg-0lax\">Luca Guastoni, Jean Rabault, Hossein Azizpour and Ricardo Vinuesa<\/td>\n<td class=\"tg-0lax\">Drag reduction in wall-bounded flows using deep reinforcement learning<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_196.pdf\" target=\"_blank\" rel=\"noopener\">196<\/a><\/td>\n<td class=\"tg-0lax\">Alex Zhelebovskiy, Guangyao Cui, Siddhartha Verma, Beni Cukurel and Ian Jacobi<\/td>\n<td class=\"tg-0lax\">Scale-Interactions in the Wake of an Actuated Cylinder<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_197.pdf\" target=\"_blank\" rel=\"noopener\">197<\/a><\/td>\n<td class=\"tg-0lax\">Justas \u0160ereika, Paulius Vilkinis and Nerijus Pedi\u0161ius<\/td>\n<td class=\"tg-0lax\">Experimental analysis of pulsatile flow in a transitional-type cavity<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_198.pdf\" target=\"_blank\" rel=\"noopener\">198<\/a><\/td>\n<td class=\"tg-0lax\">Paulius Vilkinis, Justas \u0160ereika and Nerijus Pedi\u0161ius<\/td>\n<td class=\"tg-0lax\">Investigation of flow over triangular roughness elements in a cavity<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_205.pdf\" target=\"_blank\" rel=\"noopener\">205<\/a><\/td>\n<td class=\"tg-0lax\">Giulia Piumini, Martin P. A. Assen, Detlef Lohse and Roberto Verzicco<\/td>\n<td class=\"tg-0lax\">Chirality of particles doesn\u2019t matter in strong turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_220.pdf\" target=\"_blank\" rel=\"noopener\">220<\/a><\/td>\n<td class=\"tg-0lax\">Dennis van Gils, Duco van Buuren, Gert-Wim Bruggert and Dominik Krug<\/td>\n<td class=\"tg-0lax\">A jetting grid driven by temporally and spatially coherent 4-D gradient noise<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2116\" class=\"elementor-tab-title\" data-tab=\"6\" role=\"button\" aria-controls=\"elementor-tab-content-2116\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Vortex Dynamics II. Room S05. Chair: Wouter Bos<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2116\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"6\" role=\"region\" aria-labelledby=\"elementor-tab-title-2116\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_76.pdf\" target=\"_blank\" rel=\"noopener\">76<\/a><\/td>\n<td class=\"tg-0lax\">Weiyu Shen, Jie Yao, Fazle Hussain and Yue Yang<\/td>\n<td class=\"tg-0lax\">Role of internal structures within a vortex in helicity dynamics<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_79.pdf\" target=\"_blank\" rel=\"noopener\">79<\/a><\/td>\n<td class=\"tg-0lax\">Zhaoyuan Meng, Weiyu Shen and Yue Yang<\/td>\n<td class=\"tg-0lax\">Evolution of dissipative fluid flows with imposed helicity conservation<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_114.pdf\" target=\"_blank\" rel=\"noopener\">114<\/a><\/td>\n<td class=\"tg-0lax\">Guido Boffetta, Stefano Musacchio, Andrea Mazzino and Marco Edoardo Rosti<\/td>\n<td class=\"tg-0lax\">Inverse energy cascade in confined three-dimensional turbulence<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_115.pdf\" target=\"_blank\" rel=\"noopener\">115<\/a><\/td>\n<td class=\"tg-0lax\">Zehao Wang, Xin Chen and Hengdong Xi<\/td>\n<td class=\"tg-0lax\">Evolution of flow topology with Prandtl number in turbulent Rayleigh-B\u00e9nard convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_118.pdf\" target=\"_blank\" rel=\"noopener\">118<\/a><\/td>\n<td class=\"tg-0lax\">Andrei Teimurazov, Sanjay Singh, Sylvie Su, Sven Eckert, Tobias Vogt and Olga Shishkina<\/td>\n<td class=\"tg-0lax\">The structural unit of oscillatory large-scale circulation<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_138.pdf\" target=\"_blank\" rel=\"noopener\">138<\/a><\/td>\n<td class=\"tg-0lax\">Daigaku Katsumi, Masanobu Inubushi and Naoto Yokoyama<\/td>\n<td class=\"tg-0lax\">Reservoir computing for prediction of intermittent reversals of large-scale vortex in two-dimensional thermal convection<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_141.pdf\" target=\"_blank\" rel=\"noopener\">141<\/a><\/td>\n<td class=\"tg-0lax\">Xue Chen, Yongmann Chung and Minping Wan<\/td>\n<td class=\"tg-0lax\">Evolution of near-wall backflow region in wall-bounded flows<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_148.pdf\" target=\"_blank\" rel=\"noopener\">148<\/a><\/td>\n<td class=\"tg-0lax\">Jihyeon Park, Junsung Choi, Ji Hun Song and Minsuk Choi<\/td>\n<td class=\"tg-0lax\">Effects of Nozzle Shapes and Compressibility on Formation of Synthetic Jets<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2117\" class=\"elementor-tab-title\" data-tab=\"7\" role=\"button\" aria-controls=\"elementor-tab-content-2117\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Acoustic. Room S06. Chair: Omri Ram<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2117\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"7\" role=\"region\" aria-labelledby=\"elementor-tab-title-2117\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_256.pdf\" target=\"_blank\" rel=\"noopener\">256<\/a><\/td>\n<td class=\"tg-0lax\">Alexis Duddridge, Vishal Chaugule, Callum Atkinson and Julio Soria<\/td>\n<td class=\"tg-0lax\">Dual-PIV coupled with dynamic mode decomposition to unravel the structure and dynamics of a supersonic free-jet<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_315.pdf\" target=\"_blank\" rel=\"noopener\">315<\/a><\/td>\n<td class=\"tg-0lax\">Yihong Fang and Jiaming Hu<\/td>\n<td class=\"tg-0lax\">Two mechanisms of sound radiation by instability waves on a subsonic jet<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_377.pdf\" target=\"_blank\" rel=\"noopener\">377<\/a><\/td>\n<td class=\"tg-0lax\">Luca Franceschelli, Marco Raiola and Stefano Discetti<\/td>\n<td class=\"tg-0lax\">Jet flow feature estimation with snapshot PIV and fast probes<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_384.pdf\" target=\"_blank\" rel=\"noopener\">384<\/a><\/td>\n<td class=\"tg-0lax\">Jonathan Stocking and Roger Oba<\/td>\n<td class=\"tg-0lax\">Statistics and spatio-temporal correlations of flow-induced wall pressure noise beneath an impinging round jet boundary layer<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_395.pdf\" target=\"_blank\" rel=\"noopener\">395<\/a><\/td>\n<td class=\"tg-0lax\">Lara De Broeck, Simon G\u00f6rtz, Patrick Alter, Jan Baumg\u00e4rtner and Martin Oberlack<\/td>\n<td class=\"tg-0lax\">Influence of wall impedance and temperature on the stability of turbulent high Mach number boundary layers<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_396.pdf\" target=\"_blank\" rel=\"noopener\">396<\/a><\/td>\n<td class=\"tg-0lax\">Simon Goertz, Lara De Broeck, Paul Hollmann, Jan-Benedikt Baumg\u00e4rtner, Patrick Alter and Martin Oberlack<\/td>\n<td class=\"tg-0lax\">Instability triggering by acoustic waves in a turbulent compressible shear layer<\/td>\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2118\" class=\"elementor-tab-title\" data-tab=\"8\" role=\"button\" aria-controls=\"elementor-tab-content-2118\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Transport and Mixing II. Room N01. Chair: Guillaume\tRoullet<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2118\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"8\" role=\"region\" aria-labelledby=\"elementor-tab-title-2118\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_202.pdf\" target=\"_blank\" rel=\"noopener\">202<\/a><\/td>\n<td class=\"tg-0lax\">Desmond Lim and Christina Vanderwel<\/td>\n<td class=\"tg-0lax\">Effects of crowd density on scalar dispersion in indoor spaces<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_231.pdf\" target=\"_blank\" rel=\"noopener\">231<\/a><\/td>\n<td class=\"tg-0lax\">Filipe Pereira, Samuel Pellone, Tiffany Desjardins, John Charonko and Forrest Doss<\/td>\n<td class=\"tg-0lax\">Modeling and Simulation of Materials Mixing with Practical Scale-Resolving Simulation Model<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_251.pdf\" target=\"_blank\" rel=\"noopener\">251<\/a><\/td>\n<td class=\"tg-0lax\">Sheng-Hong Peng, Yi-Bao Zhang and Heng-Dong Xi<\/td>\n<td class=\"tg-0lax\">Effects of polymer additives on the entrainment of turbulent water jet<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_257.pdf\" target=\"_blank\" rel=\"noopener\">257<\/a><\/td>\n<td class=\"tg-0lax\">Nairita Pal<\/td>\n<td class=\"tg-0lax\">The Local Wavenumber Model for Turbulent Mixing<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_279.pdf\" target=\"_blank\" rel=\"noopener\">279<\/a><\/td>\n<td class=\"tg-0lax\">Elian Bernard<\/td>\n<td class=\"tg-0lax\">Simoultaneous velocity and thermal field measurment using Thermochromic Liquid Crystal<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_280.pdf\" target=\"_blank\" rel=\"noopener\">280<\/a><\/td>\n<td class=\"tg-0lax\">Cyprien Lemar\u00e9chal, Guillaume Roullet and Jonathan Gula<\/td>\n<td class=\"tg-0lax\">Properties of vertical plumes emanating from oceanic hydrothermal springs using LES<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_297.pdf\" target=\"_blank\" rel=\"noopener\">297<\/a><\/td>\n<td class=\"tg-0lax\">Stefan S. Nixon, Stuart B. Dalziel and Romain Watteaux<\/td>\n<td class=\"tg-0lax\">Experimental detection of large-scale flow structures in a Rayleigh-Taylor instability<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-2119\" class=\"elementor-tab-title\" data-tab=\"9\" role=\"button\" aria-controls=\"elementor-tab-content-2119\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-left\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">Instability and Transition II. Room AirNostrum. Chair: Baofang Song<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-2119\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"9\" role=\"region\" aria-labelledby=\"elementor-tab-title-2119\"><table class=\"tg\">\n<tbody>\n<tr>\n<td class=\"tg-0lax\">17:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_73.pdf\" target=\"_blank\" rel=\"noopener\">73<\/a><\/td>\n<td class=\"tg-0lax\">Andrey Aleksyuk and Matthias Heil<\/td>\n<td class=\"tg-0lax\">Mechanisms for three-dimensional instabilities in the wake behind a cylinder<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_108.pdf\" target=\"_blank\" rel=\"noopener\">108<\/a><\/td>\n<td class=\"tg-0lax\">Guillaume Costa, Amaury Barral and B\u00e9reng\u00e8re Dubrulle<\/td>\n<td class=\"tg-0lax\">Simulations of reversible Navier-Stokes equation on logarithmic lattices<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:30:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_123.pdf\" target=\"_blank\" rel=\"noopener\">123<\/a><\/td>\n<td class=\"tg-0lax\">Beno\u00eet Semin, Tao Liu, Ramiro Godoy-Diana and Jos\u00e9 Eduardo Wesfreid<\/td>\n<td class=\"tg-0lax\">Dynamics of turbulent structures in Couette-Poiseuille flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">17:45:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_128.pdf\" target=\"_blank\" rel=\"noopener\">128<\/a><\/td>\n<td class=\"tg-0lax\">Artur Gesla, Laurent Martin Witkowski, Yohann Duguet and Patrick Le Qu\u00e9r\u00e9<\/td>\n<td class=\"tg-0lax\">Nonlinear dynamics of closed axisymmetric rotor-stator flow<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:00:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_147.pdf\" target=\"_blank\" rel=\"noopener\">147<\/a><\/td>\n<td class=\"tg-0lax\">Kosuke Nakagawa, Takahiro Ishida and Takahiro Tsukahara<\/td>\n<td class=\"tg-0lax\">Parametric study on the effects of cylindrical cavities on transition in the Falkner-Skan-Cooke boundary layer<\/td>\n<\/tr>\n<tr>\n<td class=\"tg-0lax\">18:15:00<\/td>\n<td class=\"tg-baqh\"><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_152.pdf\" target=\"_blank\" rel=\"noopener\">152<\/a><\/td>\n<td class=\"tg-0lax\">Tom T. B. Wester, Joachim Peinke and Gerd G\u00fclker<\/td>\n<td class=\"tg-0lax\">Description of boundary layer transition from laminar to turbulent state using directed percolation<\/td>\n<\/tr>\n<tr>\n<td>18:30:00<\/td>\n<td><a href=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/07\/ETC18_paper_425.pdf\" target=\"_blank\" rel=\"noopener\">425<\/a><\/td>\n<td>Daniel Israel<\/td>\n<td>The Myth of URANS<\/td>\n\n<\/tr>\n<\/tbody>\n<\/table><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"has_eae_slider elementor-section elementor-top-section elementor-element elementor-element-fd5bfff elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"26552\" data-id=\"fd5bfff\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"has_eae_slider elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-eee3958\" data-eae-slider=\"20825\" data-id=\"eee3958\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-cd0752b elementor-widget elementor-widget-text-editor\" data-id=\"cd0752b\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h1 style=\"text-align: center;\">Day 1 ends. See you tomorrow!<\/h1><div style=\"text-align: center;\"><a href=\"https:\/\/www.visitvalencia.com\/en\">Valencia Tourism Official Site | Visit Valencia<\/a><\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>09:15 &#8211; 09:30 Meeting inauguration NEXUS Prof. Dr. Dolores Salvador, Deputy Chancellor for Employment and Lifelong Learning 09:30 &#8211; 10:15 Keynote Speaker 1 NEXUS Soledad Le Clainche Modal decompositions and other machine learning tools in fluid dynamics 10:15 &#8211; 11:00 Keynote Speaker 2 NEXUS Shervin Bagheri Functionality and stability of liquid-infused surfaces in shear flows &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/monday-04\/\" class=\"more-link\">Read more<span class=\"screen-reader-text\"> &#8220;Monday 4th&#8221;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"inspiro_hide_title":false,"footnotes":""},"folder":[],"class_list":["post-12981","page","type-page","status-publish","hentry"],"aioseo_notices":[],"featured_media_urls":[],"_links":{"self":[{"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages\/12981","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/comments?post=12981"}],"version-history":[{"count":130,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages\/12981\/revisions"}],"predecessor-version":[{"id":14082,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages\/12981\/revisions\/14082"}],"wp:attachment":[{"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/media?parent=12981"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/folder?post=12981"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}