{"id":754,"date":"2015-10-03T05:59:44","date_gmt":"2015-10-03T03:59:44","guid":{"rendered":"http:\/\/toschi.phys.tue.nl\/wordpress\/?p=754"},"modified":"2015-10-03T06:06:42","modified_gmt":"2015-10-03T04:06:42","slug":"matteo-lulli","status":"publish","type":"post","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/matteo-lulli\/","title":{"rendered":"Matteo Lulli"},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"754\">\n<div class='content-wrap'><p><strong>Evaporation of Droplets under flow<\/strong><br \/>\n<a href=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg\"><img data-recalc-dims=\"1\" loading=\"lazy\" decoding=\"async\" data-attachment-id=\"756\" data-permalink=\"https:\/\/toschi.phys.tue.nl\/wordpress\/matteo-lulli\/matteolulli_profilepic\/\" data-orig-file=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?fit=2340%2C4160&amp;ssl=1\" data-orig-size=\"2340,4160\" data-comments-opened=\"0\" data-image-meta=\"{&quot;aperture&quot;:&quot;2.4&quot;,&quot;credit&quot;:&quot;&quot;,&quot;camera&quot;:&quot;LG-D855&quot;,&quot;caption&quot;:&quot;&quot;,&quot;created_timestamp&quot;:&quot;1419530332&quot;,&quot;copyright&quot;:&quot;&quot;,&quot;focal_length&quot;:&quot;3.97&quot;,&quot;iso&quot;:&quot;150&quot;,&quot;shutter_speed&quot;:&quot;0.058823529411765&quot;,&quot;title&quot;:&quot;&quot;,&quot;orientation&quot;:&quot;1&quot;}\" data-image-title=\"MatteoLulli_profilePic\" data-image-description=\"\" data-image-caption=\"\" data-large-file=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?fit=697%2C1239&amp;ssl=1\" class=\"alignleft size-medium wp-image-756\" src=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?resize=169%2C300\" alt=\"MatteoLulli_profilePic\" width=\"169\" height=\"300\" srcset=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?resize=169%2C300&amp;ssl=1 169w, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?resize=768%2C1365&amp;ssl=1 768w, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?resize=700%2C1244&amp;ssl=1 700w, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?w=1394 1394w, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/10\/MatteoLulli_profilePic.jpg?w=2091 2091w\" sizes=\"auto, (max-width: 169px) 100vw, 169px\" \/><\/a><\/p>\n<p>The aim of the project if to develop a stable and accurate numerical technique based on the Lattice-Boltzmann scheme to quantitatively study the diffusion behaviour of multicomponent droplets under flow. The ability of simulating correctly the diffusive dynamics of multicomponent droplets in presence of advection is per se an challenging and fundamental issue, the final purpose of the project is to develop numerical techniques suitable for the study and understanding of the so-called surface nano-droplets. These droplets are softly pinned to a substrate and their height is of the order of nanometers. They show an extremely long lifetime whose order is set by the macroscopic size of the system and by the value of the diffusion constant. From a first theoretical approach the resulting model shows a rich variety of dynamics for their dissolution.<\/p>\n<\/div><!-- kcite active, but no citations found -->\n<\/div> <!-- kcite-section 754 -->","protected":false},"excerpt":{"rendered":"<p>Evaporation of Droplets under flow The aim of the project if to develop a stable and accurate numerical technique based on the Lattice-Boltzmann scheme to quantitatively study the diffusion behaviour of multicomponent droplets under flow. The ability of simulating correctly the diffusive dynamics of multicomponent droplets in presence of advection is per se an challenging [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_exactmetrics_skip_tracking":false,"_exactmetrics_sitenote_active":false,"_exactmetrics_sitenote_note":"","_exactmetrics_sitenote_category":0,"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[45],"tags":[],"class_list":["post-754","post","type-post","status-publish","format-standard","hentry","category-postdoc"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6tiMI-ca","jetpack_likes_enabled":true,"jetpack-related-posts":[{"id":271,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/droplets-deformation-under-turbulence\/","url_meta":{"origin":754,"position":0},"title":"Droplets deformation under turbulence","author":"toschi","date":"June 6, 2013","format":false,"excerpt":"https:\/\/vimeo.com\/64156568","rel":"","context":"In &quot;ongoing work&quot;","block_context":{"text":"ongoing work","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/research\/ongoing-work\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":307,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/cost-action-mp0806-particles-in-turbulence\/","url_meta":{"origin":754,"position":1},"title":"COST Action MP0806 \"Particles in turbulence\"","author":"toschi","date":"June 6, 2013","format":false,"excerpt":"http:\/\/mp0806.cineca.it Memorandum of understanding Fluid turbulence is ubiquitous and so is its ability to transport particulate matter such as dust, soot or droplets. The dynamics of particles in a turbulent flow is fundamental to everyday life - examples of open scientific and technological issues include rain formation in clouds, pollution\u2026","rel":"","context":"In &quot;projects&quot;","block_context":{"text":"projects","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/research\/projects\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":469,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/abhineet-gupta\/","url_meta":{"origin":754,"position":2},"title":"Abhineet Gupta","author":"toschi","date":"December 1, 2013","format":false,"excerpt":"Photo-bioreactors: saving algae from turbulence! Understanding turbulent flow of (dense) suspensions is one of the key factors needed in order to upscale and thus increase the productivity of algae photo-bioreactors. Many studies investigated the rheology of dense suspensions in laminar flows, as well as the dynamics of dilute suspensions in\u2026","rel":"","context":"In &quot;ph.d.&quot;","block_context":{"text":"ph.d.","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/students\/ph-d\/"},"img":{"alt_text":"gupta","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/12\/gupta-300x300.jpg?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":208,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/advanced-computational-fluid-dynamics\/","url_meta":{"origin":754,"position":3},"title":"3T380 - Advanced Computational Fluid Dynamics","author":"toschi","date":"February 8, 2012","format":false,"excerpt":"Quick links:\u00a0[Link to course schedule]\u00a0[Link to lecture notes]\u00a0[Link to additional books and material]\u00a0[Link to exercises]\u00a0[Link to possible individual assignments] The\u00a03T380\u00a0course provides an introduction to advanced computational methods useful to investigate fluid flows from the micro to the macro-scales under laminar and turbulent flow regime. The course will present an overview\u2026","rel":"","context":"In &quot;master&quot;","block_context":{"text":"master","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/teaching\/master\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":456,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/francesca-tesser\/","url_meta":{"origin":754,"position":4},"title":"Francesca Tesser","author":"toschi","date":"December 1, 2013","format":false,"excerpt":"Title Population dynamics under flow Aim Simulations and experiments on populations of organisms living in aquatic environments and growing under flow conditions. Summary Ocean, rivers and lakes are natural environments for many living organisms. In these ecosystems they reproduce, compete for food, swim and die. The presence of a flow\u2026","rel":"","context":"In &quot;ph.d.&quot;","block_context":{"text":"ph.d.","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/students\/ph-d\/"},"img":{"alt_text":"IMG_2391_adjust","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/12\/IMG_2391_adjust-236x300.jpg?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":262,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/convection-in-multiphase-fluid-flows-using-lattice-boltzmann-methods\/","url_meta":{"origin":754,"position":5},"title":"Convection in multiphase fluid flows using lattice Boltzmann methods","author":"toschi","date":"June 6, 2013","format":false,"excerpt":"Biferale, L., Perlekar, P., Sbragaglia, M. & Toschi, F. (2012). Convection in multiphase fluid flows using lattice Boltzmann methods. Physical Review Letters, 108(10):104502 DOI We present high-resolution numerical simulations of convection in multiphase flows (boiling) using a novel algorithm based on a lattice Boltzmann method. We first study the thermodynamical\u2026","rel":"","context":"In \"heat transfer\"","block_context":{"text":"heat transfer","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/tag\/heat-transfer\/"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/screen.png?fit=953%2C939&ssl=1&resize=350%2C200","width":350,"height":200,"srcset":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/screen.png?fit=953%2C939&ssl=1&resize=350%2C200 1x, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/screen.png?fit=953%2C939&ssl=1&resize=525%2C300 1.5x, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/screen.png?fit=953%2C939&ssl=1&resize=700%2C400 2x"},"classes":[]}],"_links":{"self":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/754","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/comments?post=754"}],"version-history":[{"count":3,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/754\/revisions"}],"predecessor-version":[{"id":758,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/754\/revisions\/758"}],"wp:attachment":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/media?parent=754"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/categories?post=754"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/tags?post=754"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}