{"id":62,"date":"2017-07-01T13:44:03","date_gmt":"2017-07-01T13:44:03","guid":{"rendered":"http:\/\/wp.df.uba.ar\/flip\/?page_id=62"},"modified":"2024-03-09T17:44:56","modified_gmt":"2024-03-09T17:44:56","slug":"soft-matter","status":"publish","type":"page","link":"http:\/\/wp.df.uba.ar\/flip\/soft-matter\/","title":{"rendered":"Soft matter"},"content":{"rendered":"\n<p><strong>Generation of droplets: <\/strong>In the geophysical turbulence laboratory, under the supervision of Pablo Cobelli, we also design and develop systems to generate droplets of controlled size. These are used in multiple experiments, to study interaction of droplets with surface waves, as well as for industrial applications.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"451\" src=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplet1-1024x451.jpg\" alt=\"\" class=\"wp-image-100\" srcset=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplet1-1024x451.jpg 1024w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplet1-300x132.jpg 300w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplet1-768x338.jpg 768w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplet1.jpg 1262w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n<\/div>\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity is-style-wide\" \/>\n\n\n\n<p><strong>Flow-particle interactions:<\/strong> In the laboratory Pablo Cobelli studies bouncing droplets, the interaction of surface waves with obstacles with applications in the study of <a href=\"https:\/\/hal-polytechnique.archives-ouvertes.fr\/hal-01657084\/document\" target=\"_blank\" rel=\"noreferrer noopener\">metamaterials<\/a>, the <a href=\"https:\/\/www.pmmh.espci.fr\/~phil\/Articles\/art_73.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">interaction of surface waves with bottom topography and deformation<\/a>, <a href=\"https:\/\/arxiv.org\/pdf\/1301.1024.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">soft interfaces<\/a>, propagation of waves in foams, transport of particles by surface deformations in a liquid, and <a href=\"https:\/\/journals.aps.org\/prfluids\/abstract\/10.1103\/PhysRevFluids.5.064605\" target=\"_blank\" rel=\"noreferrer noopener\">multi-phase turbulent flows<\/a>.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"583\" src=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplets2-1024x583.jpg\" alt=\"\" class=\"wp-image-101\" srcset=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplets2-1024x583.jpg 1024w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplets2-300x171.jpg 300w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplets2-768x437.jpg 768w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/droplets2.jpg 1184w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n<\/div>\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity is-style-wide\" \/>\n\n\n\n<p><strong>Instrumented particles:<\/strong> To measure Lagrangian acceleration of particles in surface wave turbulence we are also developing instrumented particles that can transmit or record acceleration and particle orientation as a function of time. Such particles can be used for the <a href=\"https:\/\/link.springer.com\/article\/10.1007\/s00348-020-03121-3\" target=\"_blank\" rel=\"noreferrer noopener\">characterization of Lagrangian properties of wave turbulence<\/a>, as found in the ocean and in laboratory experiments.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"768\" src=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/IMG_6061-2-1024x768.jpg\" alt=\"\" class=\"wp-image-102\" srcset=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/IMG_6061-2-1024x768.jpg 1024w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/IMG_6061-2-300x225.jpg 300w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/IMG_6061-2-768x576.jpg 768w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n<\/div>\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity is-style-wide\" \/>\n\n\n\n<p><strong>Quantum turbulence:<\/strong> Quantum turbulence is the disorganized flow state observed in superfluids and Bose-Einstein condensates. Unlike classical flows, quantum flows have no viscosity, and vorticity is concentrated along topological line defects with quantized circulation. While similarities between classical and quantum turbulence exist, there are also important differences. In our group we study quantum turbulence in numerical simulations, solving the Gross-Pitaevskii equation, as well as other models for finite temperature condensates such as truncated equations and the Stochastic Ginzburg-Landau equations. Recently we studied <a href=\"https:\/\/arxiv.org\/pdf\/1509.05316.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">the role of Kelvin waves<\/a> in quantum turbulence, we considered the evolution of <a href=\"https:\/\/arxiv.org\/pdf\/1602.06880.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">helicity in quantum knots<\/a>, dual cascades and dissipation mechanism in <a href=\"https:\/\/arxiv.org\/pdf\/1705.03525.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">helical quantum turbulence<\/a> (using numerical simulations with up to 2048<sup>3<\/sup> grid points), and <a href=\"https:\/\/arxiv.org\/pdf\/1711.08614.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">finite temperature effects in helical quantum turbulence<\/a> (using simulations with 4096<sup>3<\/sup> grid points).<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"613\" src=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/quantum-1024x613.jpg\" alt=\"\" class=\"wp-image-99\" srcset=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/quantum-1024x613.jpg 1024w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/quantum-300x180.jpg 300w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/quantum-768x460.jpg 768w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2018\/01\/quantum.jpg 2000w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n<\/div>\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity is-style-wide\" \/>\n\n\n\n<p><strong>Quantum fluids and Bose-Einstein condensates:<\/strong> We study thermodynamic and out-of equilibrium properties of quantum fluids, with a special emphasis on theoretical and numerical descriptions based on the non-linear Schr\u00f6dinger equation. These studies include the <a href=\"https:\/\/pubs.aip.org\/avs\/aqs\/article\/4\/4\/046201\/2835283\/Thermalized-Abrikosov-lattices-from-decaying\" target=\"_blank\" rel=\"noreferrer noopener\">dynamics of rotating Bose-Einstein condensates<\/a>, applications of mean field descriptions of quantum fluids to <a href=\"https:\/\/arxiv.org\/pdf\/2204.07260\" target=\"_blank\" rel=\"noreferrer noopener\">superconductivity<\/a>, and the <a href=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.109.012202\" data-type=\"link\" data-id=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.109.012202\">thermodynamics of quantum thermal machines<\/a>.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"504\" src=\"https:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-1024x504.jpg\" alt=\"\" class=\"wp-image-190\" srcset=\"http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-1024x504.jpg 1024w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-300x148.jpg 300w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-768x378.jpg 768w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-1536x756.jpg 1536w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec-150x74.jpg 150w, http:\/\/wp.df.uba.ar\/flip\/wp-content\/uploads\/sites\/15\/2023\/05\/bec.jpg 1721w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>Generation of droplets: In the geophysical turbulence laboratory, under the supervision of Pablo Cobelli, we also design and develop systems to generate droplets of controlled size. These are used in multiple experiments, to study interaction of droplets with surface waves, as well as for industrial applications. Flow-particle interactions: In the laboratory Pablo Cobelli studies bouncing &hellip; <\/p>\n<p class=\"link-more\"><a href=\"http:\/\/wp.df.uba.ar\/flip\/soft-matter\/\" class=\"more-link\">Continuar leyendo<span class=\"screen-reader-text\"> &#8220;Soft matter&#8221;<\/span><\/a><\/p>\n","protected":false},"author":18,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_bbp_topic_count":0,"_bbp_reply_count":0,"_bbp_total_topic_count":0,"_bbp_total_reply_count":0,"_bbp_voice_count":0,"_bbp_anonymous_reply_count":0,"_bbp_topic_count_hidden":0,"_bbp_reply_count_hidden":0,"_bbp_forum_subforum_count":0,"footnotes":""},"class_list":["post-62","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/pages\/62","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/users\/18"}],"replies":[{"embeddable":true,"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/comments?post=62"}],"version-history":[{"count":3,"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/pages\/62\/revisions"}],"predecessor-version":[{"id":207,"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/pages\/62\/revisions\/207"}],"wp:attachment":[{"href":"http:\/\/wp.df.uba.ar\/flip\/wp-json\/wp\/v2\/media?parent=62"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}