{"id":12612,"date":"2023-01-08T12:17:55","date_gmt":"2023-01-08T12:17:55","guid":{"rendered":"https:\/\/etc18.webs.upv.es\/?page_id=12612"},"modified":"2023-05-16T15:15:45","modified_gmt":"2023-05-16T15:15:45","slug":"keynote","status":"publish","type":"page","link":"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/","title":{"rendered":"Keynote Speakers"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"12612\" class=\"elementor elementor-12612\" 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-1fe8bce elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"45318\" data-id=\"1fe8bce\" 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-52e3ad1\" data-eae-slider=\"57450\" data-id=\"52e3ad1\" 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-d0a788d elementor-widget elementor-widget-heading\" data-id=\"d0a788d\" 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<h1 class=\"elementor-heading-title elementor-size-default\">Keynote Speakers<\/h1>\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-98985c9 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"61664\" data-id=\"98985c9\" 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-33 elementor-top-column elementor-element elementor-element-dc91292\" data-eae-slider=\"84679\" data-id=\"dc91292\" 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-f396abb elementor-widget elementor-widget-image\" data-id=\"f396abb\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"300\" height=\"226\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/csm_MarcAvila2020_398f67e6a8.jpg\" class=\"attachment-large size-large wp-image-12635\" alt=\"\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-882305e\" data-eae-slider=\"44147\" data-id=\"882305e\" 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-6d17f6a elementor-widget elementor-widget-text-editor\" data-id=\"6d17f6a\" 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 id=\"avila\">Marc Avila<\/h2>\n<h4>Title:\u00a0Drop breakup in turbulent flows<\/h4>\n<h4><\/h4>\n<h4>Abstract:<\/h4>\n<p class=\"MsoNormal\"><span lang=\"EN-GB\">The breakup of drops and bubbles in turbulent fluids is a key mechanism in many environmental and engineering processes, including the emulsification of immiscible liquids, sprays, rainfall and the liquid-gas exchange at the ocean-atmosphere interface. Even in the well-studied dilute case, quantitative descriptions of drop fragmentation remain elusive, and many empirical models have been proposed to date. In this talk, I will show that in homogeneous isotropic turbulence, drop breakup is a memoryless process. The corresponding time constant increases exponentially as the Weber number decreases. As a consequence, dilute emulsions evolve through a continuous fragmentation process with exponentially increasing time scales. I\u2019ll conclude the talk by demonstrating that breakup is caused by outer eddies capable of generating strain at the drop surface by virtue of the non-local coupling between vorticity and strain rate. Modelling approaches exploiting this finding will be discussed in the context of extreme (rare) events in turbulence, drawing an analogy to turbulence transition in pipe flow.\u00a0<\/span><span style=\"color: var( --e-global-color-text ); font-family: var( --e-global-typography-text-font-family ), Sans-serif; font-weight: var( --e-global-typography-text-font-weight );\">The presented work has been done together with Alberto Vela Mart\u00edn.\u00a0<\/span><\/p>\n\n<h4>Biography:<\/h4>\n<p class=\"MsoNormal\" style=\"text-align: justify;\">Marc Avila studied Mathematics at the Universitat Aut\u00f2noma de Barcelona\u00a0and at the University of Glasgow and got his PhD in Applied Physics and\u00a0Scientific Computing from the Universitat Polit\u00e8cnica de Catalunya in 2008.\u00a0During his PhD, he was a research scholar at the Arizona State University and\u00a0subsequently a postdoc at the Max-Planck-Institute for Dynamics and Self-Organization.\u00a0Prior to becoming Professor of fluid mechanics at the University of Bremen, and\u00a0Director of its Center of Applied Space Technology and Microgravity (ZARM), he\u00a0was Professor at the University of Erlangen-Nuremberg. For his work on the\u00a0transition to turbulence in pipe flow, he received the Euromech Young Scientist\u00a0Award in 2009 and the <span lang=\"EN-GB\">Richard-von-Mises\u00a0Prize of the GAMM in 2018. He enjoys applying dynamical-systems approaches to\u00a0understand and predict the dynamics of transitional and turbulent flows, and\u00a0more recently of multiphase flows.\u00a0\u00a0<\/span><\/p>\n&nbsp;\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-c90f0d9 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"35516\" data-id=\"c90f0d9\" 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-1ad5dcf\" data-eae-slider=\"64472\" data-id=\"1ad5dcf\" 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-39c5ed9 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"39c5ed9\" 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-371f03c elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"57849\" data-id=\"371f03c\" 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-33 elementor-top-column elementor-element elementor-element-1b8d83c\" data-eae-slider=\"80200\" data-id=\"1b8d83c\" 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-eced6ce elementor-widget elementor-widget-image\" data-id=\"eced6ce\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"239\" height=\"320\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/bagheri.png\" class=\"attachment-large size-large wp-image-12632\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/bagheri.png 239w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/bagheri-224x300.png 224w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-b51b721\" data-eae-slider=\"81963\" data-id=\"b51b721\" 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-3cc95ce elementor-widget elementor-widget-text-editor\" data-id=\"3cc95ce\" 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 id=\"bagheri\">Shervin Bagheri<\/h2>\n<h4>Title: Functionality and stability of liquid-infused surfaces in shear flows<\/h4>\n<h4><\/h4>\n<h4>Abstract:<\/h4>\n<span style=\"font-size: 11.0pt; font-family: 'Calibri',sans-serif; mso-fareast-font-family: 'Times New Roman'; mso-ansi-language: EN-US; mso-fareast-language: EN-US; mso-bidi-language: AR-SA;\">Robust surfaces that can resist fouling, reduce flow drag, and control heat and mass transfer in turbulent flows would have broad technological implications. In this talk, I will focus on how lubricant-infused surfaces (LIS) can be used to control turbulent transport processes. LIS are slippery surfaces that use microstructures to lock in place a lubricating liquid. Under gentle conditions, they have already demonstrated anti-fouling, drag reduction, and heat transfer enhancement. However, when submerged in turbulent flows, these surfaces drastically change their behavior. The lubricant-liquid interface can break up and partially drain, resulting in complex patterns. It can sustain large capillary waves, leading to surface roughness.\u00a0\u00a0It can also change or acquire new properties from Marangoni stresses, induced by surfactants or temperature variations. I will discuss how these phenomena originate from flow-induced instabilities of liquid-liquid interfaces and how they modify turbulent transport processes.&#8221;<\/span>\n<h4>Biography:<\/h4>\n<p style=\"text-align: justify;\">Professor Bagheri\u2019s research focuses on the interaction between flowing fluids and complex materials across different length and time scales, ranging from molecular aspects of triple-phase contact lines to turbulent flows over porous media. His main objective is to apply this understanding to control\/sense flows and transport phenomenas. Shervin Bagheri received his PhD in Fluid Mechanics at Royal Institute of Technology (KTH) in Stockholm in 2010. In 2017, he was appointed as Wallenberg Academy Fellow and received the Future Research Leader award by Swedish Foundation for Strategic research (SSF). Since 2020, he is a member of the Young Academy of Sweden. In 2022, he received ERC Consolidator grant for studying lubricated surfaces in fluid flows.<\/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\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-cce4cbe elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"82179\" data-id=\"cce4cbe\" 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-aeda9e2\" data-eae-slider=\"51419\" data-id=\"aeda9e2\" 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-e8e715f elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"e8e715f\" 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-0fe8e08 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"92535\" data-id=\"0fe8e08\" 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-33 elementor-top-column elementor-element elementor-element-d8e7251\" data-eae-slider=\"62930\" data-id=\"d8e7251\" 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-0375aab elementor-widget elementor-widget-image\" data-id=\"0375aab\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"353\" height=\"393\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/leonie-canet-portrait.png\" class=\"attachment-large size-large wp-image-12634\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/leonie-canet-portrait.png 353w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/leonie-canet-portrait-269x300.png 269w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-b31aa6a\" data-eae-slider=\"64556\" data-id=\"b31aa6a\" 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-ca8aebf elementor-widget elementor-widget-text-editor\" data-id=\"ca8aebf\" 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 id=\"canet\">Leonie Canet<\/h2>\n<h4>Title:\u00a0 Functional renormalisation group approach to turbulence<\/h4>\n<h4>Abstract:<\/h4>\n<p style=\"text-align: justify;\">The aim of this talk is to give an overview of the results which can be obtained on the statistical properties of turbulence using a specific implementation of the Renormalisation Group (RG) called Non-perturbative or Functional RG. I will focus on isotropic, homogeneous and stationary turbulence in incompressible flows, and also on passive scalar turbulence. I will first briefly introduce the FRG formalism to study the Navier-Stokes equation and turbulence, and describe the RG fixed-point corresponding to stationary turbulence with large-scale forcing. I will then show that the FRG allows one to obtain analytical results on the space-time dependence of generic multi-point correlation functions of the turbulent velocity in the limit of large wavenumbers. I will compare these predictions with available results from direct numerical simulations and experiments. I will finally discuss the FRG analysis of shell models of turbulence.<\/p>\n\n<h4>Biography:<\/h4>\n<p style=\"text-align: justify;\"><span style=\"font-kerning: none;\">L\u00e9onie Canet is a Professor at University Grenoble Alpes and she is also a member of the Institut Universitaire de France since 2019. She received her PhD in theoretical physics in 2004 in Paris, and her main area of research is statistical physics, in particular the theoretical study of classical non-equilibrium systems and non-equilibrium critical phenomena, and also open quantum systems and driven-dissipative Bose-Einstein condensates. She is an expert in functional and non-perturbative renormalisation group methods. She was awarded the Bronze medal of CNRS in 2018.<\/span><\/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\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-ad4eadb elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"70165\" data-id=\"ad4eadb\" 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-35fda27\" data-eae-slider=\"81240\" data-id=\"35fda27\" 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-c2fae50 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"c2fae50\" 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-5a26c79 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"87568\" data-id=\"5a26c79\" 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-33 elementor-top-column elementor-element elementor-element-6bbb6fa\" data-eae-slider=\"61004\" data-id=\"6bbb6fa\" 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-5cdb477 elementor-widget elementor-widget-image\" data-id=\"5cdb477\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"628\" height=\"629\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/massimocencini.jpg\" class=\"attachment-large size-large wp-image-12633\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/massimocencini.jpg 628w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/massimocencini-300x300.jpg 300w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/massimocencini-150x150.jpg 150w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/massimocencini-600x601.jpg 600w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-9ea03fd\" data-eae-slider=\"78702\" data-id=\"9ea03fd\" 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-c920fef elementor-widget elementor-widget-text-editor\" data-id=\"c920fef\" 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 id=\"cencini\">Massimo Cencini<\/h2>\n<h4>Title:\u00a0<span style=\"font-kerning: none;\"> Microorganisms swimming in turbulence<\/span><\/h4>\n<h4>Abstract:<\/h4>\n<p style=\"text-align: justify;\"><span style=\"font-kerning: none;\">Many aquatic microorganisms are motile from bacteria to several species of phytoplankton. The complex interplay between fluid transport, motility and shape of the microswimmers can give rise to non-trivial spatial organization and orientation dynamics for the microorganisms. I will review a few studies showing the richness of behavior and how simple mechanistic models for the microswimmers motility allow to account for several phenomena<\/span><\/p>\n\n<h4>Biography:<\/h4>\n<p style=\"text-align: justify;\"><span style=\"font-kerning: none;\">Massimo Cencini is senior researcher at the Institute of Complex Systems\u00a0of the Italian National Research Council (CNR). He received his PhD in Physics from the University\u00a0of Rome\u00a0\u201cLa Sapienza\u201d in 2000. He has been post-doc at the Max Planck Institute for Complex Systems in Dresden (Germany) and at the Observatory of the Cote d\u2019Azur in Nice (France). The leading themes of his research activity are dynamical systems, statistical theories of turbulence and turbulent transport and, more recently, the study of the interplay between fluid transport and motility of microswimmers.<\/span><\/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\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-ab51953 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"71213\" data-id=\"ab51953\" 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-179a6da\" data-eae-slider=\"28889\" data-id=\"179a6da\" 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-11ab2bc elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"11ab2bc\" 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-f28b0df elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"84863\" data-id=\"f28b0df\" 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-33 elementor-top-column elementor-element elementor-element-f7a670f\" data-eae-slider=\"29390\" data-id=\"f7a670f\" 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-0b61004 elementor-widget elementor-widget-image\" data-id=\"0b61004\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"722\" height=\"646\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/PIC_sole_3.jpeg\" class=\"attachment-large size-large wp-image-12631\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/PIC_sole_3.jpeg 722w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/PIC_sole_3-300x268.jpeg 300w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/PIC_sole_3-600x537.jpeg 600w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-be7de45\" data-eae-slider=\"34834\" data-id=\"be7de45\" 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-4148479 elementor-widget elementor-widget-text-editor\" data-id=\"4148479\" 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 id=\"leclainche\">Soledad Le Clainche<\/h2>\n<h4 style=\"text-align: justify;\">Title: Modal decompositions and other machine learning tools in fluid\ndynamics<\/h4>\n<h4 style=\"text-align: justify;\">Abstract:<\/h4>\n<p style=\"text-align: justify;\">One of the biggest challenges our society faces is to combat climate change. To mitigate its\u00a0effects, it is necessary to explore different alternatives and develop new technologies that are\u00a0capable of reducing atmospheric pollution. Fluid mechanics is a science with multiple\u00a0applications that can be used for this purpose, such as improving combustion system efficiency,\u00a0studying ways to reduce air pollution in urban areas, and enhancing the design of aircraft and\u00a0making them more efficient. To study these issues, reduced-order models (ROMs) based on\u00a0physical principles are proposed, using (i) modal decompositions (singular value decomposition\u2013 SVD, higher-order dynamic mode decomposition &#8211; HODMD), and (ii) machine learning tools\u00a0(neural networks) combined with these decompositions. This work applies these techniques to\u00a0solve the aforementioned problems, while also presenting new strategies to develop efficient\u00a0and accurate ROMs. Additionally, a novel method fully data-driven to identify the structural\u00a0sensitivity in complex flows (fully non-linear) will be introduced. The method is based on\u00a0HODMD, and new applications for flow control will be presented.<\/p>\n\n<h4 style=\"text-align: justify;\">Biography:<\/h4>\n<p style=\"text-align: justify;\">Dr. Soledad Le Clainche is Professor of Applied Mathematics at the School of Aeronautics of the Universidad Polit\u00e9cnica de Madrid (UPM). In December 2013, she finished her Ph.D. at the same University, in the Dept. of Fluid Dynamics and Aerospace Propulsion. Her main lines of research focus on computational fluid dynamics, data analysis, machine learning, and the development and application of predictive reduced order models based on physical principles. In this line, she is the PI of several national and EU-funded projects whose main objective is to develop new strategies to reduce air pollution in cities, to develop more efficient combustion systems and aerodynamic designs, and to advance in the field of personalized medicine.<\/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\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-95bc34a elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"94912\" data-id=\"95bc34a\" 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-3942d00\" data-eae-slider=\"39740\" data-id=\"3942d00\" 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-d7d7587 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"d7d7587\" 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-054b1ae elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"93071\" data-id=\"054b1ae\" 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-33 elementor-top-column elementor-element elementor-element-4b1c889\" data-eae-slider=\"26115\" data-id=\"4b1c889\" 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-5e01152 elementor-widget elementor-widget-image\" data-id=\"5e01152\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"395\" height=\"553\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/02\/Foto.jpg\" class=\"attachment-large size-large wp-image-12677\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/02\/Foto.jpg 395w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/02\/Foto-214x300.jpg 214w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-f18260d\" data-eae-slider=\"71694\" data-id=\"f18260d\" 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-ae8a180 elementor-widget elementor-widget-text-editor\" data-id=\"ae8a180\" 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 id=\"salvetti\">Maria Vittoria Salvetti<\/h2>\n<h4 style=\"text-align: justify;\">Title: Dynamics of separating and reattaching flows<\/h4>\n<h4 style=\"text-align: justify;\">Abstract:<\/h4>\n<p style=\"text-align: justify;\">Several flow configuration of interest for engineering and environmental applications are characterized by separating and reattaching flows. An example is the flow around elongated bluff bodies, which may be considered as simplified models for high-rise buildings or bridge sections. A typical scenario is the separation of shear-layers, which undergo to instability leading to the formation of vortical structures. These structures are convected downstream interacting each other and with the solid wall. The corresponding mean flow is characterized by a recirculation region ending by mean flow reattachment. Turbulence transition and turbulence superpose to this scenario. Experimental and numerical studies are reviewed herein, to provide insights on the dynamics of separating and reattaching flows and how it impacts on the whole flow features. Implications for numerical simulations and modeling are also highlighted.<\/p>\n\n<h4 style=\"text-align: justify;\">Biography:<\/h4>\n<p style=\"text-align: justify;\">Maria Vittoria Salvetti is Full Professor of Fluid Dynamics at the Industrial and Civil Engineering Department of the University of Pisa. She is currently the Department Head.<\/p>\n<p style=\"text-align: justify;\">She is coordinator of the Special Interest Group on &#8220;Large-Eddy Simulation&#8221; (SIG 1) and chairman of the Scientific Programme Committee of the European Research Community on Flow, Turbulence and Combustion. She is member of the EUROMECH Council, of the IUTAM Congress Committee and of the Scientific Committee of Italian Space Agency. She is associated editor of Computers and Fluids and of Flow, Turbulence and Combustion, editor of the ERCOFTAC Book Series (Springer) and member of the advisory board of Acta Mechanica; she has been and is currently member of the organizing and scientific committees of many international conferences (e.g., DLES, ETMM, FRONTUQ, TI series).<\/p>\n<p style=\"text-align: justify;\">Her main research topics are: simulation and modeling, with special focus on Large-Eddy Simulation, of turbulent flows (bluff-body flows, particle-laden flows, wind turbines\u2026), reduced-order models for fluid dynamics, flow instability, flow control, drag reduction, uncertainty quantification and stochastic sensitivity analysis in CFD, micro-fluidics, cardiovascular flows.<\/p>\n<p style=\"text-align: justify;\">She is author of more than 160 scientific publications indexed in Scopus.<\/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\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-cb491e5 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"88850\" data-id=\"cb491e5\" 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-08f62ab\" data-eae-slider=\"48848\" data-id=\"08f62ab\" 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-48f8e91 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"48f8e91\" 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-4fbaa1d elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"61476\" data-id=\"4fbaa1d\" 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-33 elementor-top-column elementor-element elementor-element-cbbf8d2\" data-eae-slider=\"90678\" data-id=\"cbbf8d2\" 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-b892894 elementor-widget elementor-widget-image\" data-id=\"b892894\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"768\" height=\"1024\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-768x1024.jpg\" class=\"attachment-large size-large wp-image-12614\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-768x1024.jpg 768w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-225x300.jpg 225w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-1152x1536.jpg 1152w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-1536x2048.jpg 1536w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018-600x800.jpg 600w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/RicardoVinuesa2018.jpg 1705w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-783bd67\" data-eae-slider=\"79278\" data-id=\"783bd67\" 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-66a8523 elementor-widget elementor-widget-text-editor\" data-id=\"66a8523\" 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 id=\"vinuesa\">Ricardo Vinuesa<\/h2>\n<h4 style=\"text-align: justify;\">Title: Modeling and controlling turbulent flows through deep learning<\/h4>\n<h4 style=\"text-align: justify;\">Abstract:<\/h4>\n<p style=\"text-align: justify;\">The advent of new powerful deep neural networks (DNNs) has fostered their application in a wide range of research areas, including more recently in fluid mechanics. In this presentation, we will cover some of the fundamentals of deep learning applied to computational fluid dynamics (CFD). Furthermore, we explore the capabilities of DNNs to perform various predictions in turbulent flows: we will use convolutional neural networks (CNNs) for non-intrusive sensing, i.e. to predict the flow in a turbulent open channel based on quantities measured at the wall. We show that it is possible to obtain very good flow predictions, outperforming traditional linear models, and we showcase the potential of transfer learning between friction Reynolds numbers of 180 and 550. We also discuss other modelling methods based on autoencoders (AEs) and generative adversarial networks (GANs), and we present results of deep-reinforcement-learning-<wbr \/>based flow control.<\/p>\n\n<h4 style=\"text-align: justify;\">Biography:<\/h4>\n<p style=\"text-align: justify;\">Dr. Ricardo Vinuesa is an Associate Professor at the Department of Engineering Mechanics, at KTH Royal Institute of Technology in Stockholm. He is also Vice Director of the KTH Digitalization Platform and Lead Faculty at the KTH Climate Action Centre. He studied Mechanical Engineering at the Polytechnic University of Valencia (Spain), and he received his PhD in Mechanical and Aerospace Engineering from the Illinois Institute of Technology in Chicago. His research combines numerical simulations and data-driven methods to understand and model complex wall-bounded turbulent flows, such as the boundary layers developing around wings and urban environments. Dr. Vinuesa has received, among others, an ERC Consolidator Grant, the G\u00f6ran Gustafsson Award for Young Researchers and he is the PI of several EU-funded projects.<\/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\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-4b54b2f elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"2586\" data-id=\"4b54b2f\" 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-67a02f7\" data-eae-slider=\"32636\" data-id=\"67a02f7\" 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-9a36463 elementor-widget-divider--view-line elementor-widget elementor-widget-divider\" data-id=\"9a36463\" 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-70a7be5 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-eae-slider=\"60462\" data-id=\"70a7be5\" 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-33 elementor-top-column elementor-element elementor-element-19ce85a\" data-eae-slider=\"93743\" data-id=\"19ce85a\" 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-3898385 elementor-widget elementor-widget-image\" data-id=\"3898385\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"400\" height=\"400\" src=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/zMFDbVb7_400x400.jpg\" class=\"attachment-large size-large wp-image-12619\" alt=\"\" srcset=\"https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/zMFDbVb7_400x400.jpg 400w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/zMFDbVb7_400x400-300x300.jpg 300w, https:\/\/etc18.webs.upv.es\/wp-content\/uploads\/2023\/01\/zMFDbVb7_400x400-150x150.jpg 150w\" sizes=\"100vw\" \/>\t\t\t\t\t\t\t\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-66 elementor-top-column elementor-element elementor-element-2d1901c\" data-eae-slider=\"28488\" data-id=\"2d1901c\" 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-0edcd48 elementor-widget elementor-widget-text-editor\" data-id=\"0edcd48\" 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 id=\"williams\">Paul Williams:<\/h2>\n<div style=\"text-align: justify;\">\n<h4>Title: Forecasting atmospheric turbulence from hours to decades ahead<\/h4>\n<\/div>\n<h4 style=\"text-align: justify;\">Abstract:<\/h4>\n<p style=\"text-align: justify;\">It is well known that the atmosphere exhibits turbulence with a -5\/3 energy spectrum on small scales (on the order of 100 km and smaller).\u00a0 It is also well known (especially to airline passengers) that transient localised enhancements to this background turbulence are hazardous to aircraft.\u00a0 Understanding this aviation-affecting subset of turbulence is an important and challenging application of fluid dynamics.\u00a0 This talk will describe a new theory and mechanism for the generation of aviation turbulence.\u00a0 It will also test the skill of the mechanism by comparing observations of turbulence with predictions made from the theory.\u00a0 These tests are successful, to the extent that the algorithm is now being used operationally to predict turbulence for the aviation sector every day.\u00a0 Finally, I will explain why climate change is strengthening aviation turbulence, potentially leading to bumpier flights in future.<\/p>\n\n<h4 style=\"font-size: 16px; text-align: justify;\">Biography:<\/h4>\n<p style=\"text-align: justify;\">Paul Williams\u00a0is Professor of Atmospheric Science at the University of Reading, UK.\u00a0 Educated in physics to PhD level at Oxford, he specialises in atmospheric turbulence, jet streams, numerical modelling, and climate change.\u00a0 Regarding the effects of turbulence on commercial aircraft, he has developed award-winning turbulence forecasting algorithms that are now used operationally, and he has pioneered research into the effects of climate change on turbulence.\u00a0 He is a Fellow of the Institute of Physics and the Royal Meteorological Society.<\/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\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Keynote Speakers Marc Avila Title:\u00a0Drop breakup in turbulent flows Abstract: The breakup of drops and bubbles in turbulent fluids is a key mechanism in many environmental and engineering processes, including the emulsification of immiscible liquids, sprays, rainfall and the liquid-gas exchange at the ocean-atmosphere interface. Even in the well-studied dilute case, quantitative descriptions of drop &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/etc18.webs.upv.es\/index.php\/keynote\/\" class=\"more-link\">Read more<span class=\"screen-reader-text\"> &#8220;Keynote Speakers&#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-12612","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\/12612","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=12612"}],"version-history":[{"count":34,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages\/12612\/revisions"}],"predecessor-version":[{"id":12784,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/pages\/12612\/revisions\/12784"}],"wp:attachment":[{"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/media?parent=12612"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/etc18.webs.upv.es\/index.php\/wp-json\/wp\/v2\/folder?post=12612"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}