{"id":18969,"date":"2018-03-09T09:07:46","date_gmt":"2018-03-09T09:07:46","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/modelos-para-la-hidrodinamica-mesoscopica-de-fluidos-simples-y-complejos\/"},"modified":"2018-03-09T09:07:46","modified_gmt":"2018-03-09T09:07:46","slug":"modelos-para-la-hidrodinamica-mesoscopica-de-fluidos-simples-y-complejos","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/modelos-para-la-hidrodinamica-mesoscopica-de-fluidos-simples-y-complejos\/","title":{"rendered":"Modelos para la hidrodin\u00e1mica mesosc\u00f3pica de fluidos simples y complejos"},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Serrano Maestro M. Mar <\/strong><\/h2>\n<p>El objetivo principal de esta tesis doctoral es la fundamentaci\u00f3n de t\u00e9cnicas de simulaci\u00f3n y modelos hidrodin\u00e1micos adecuados para la simulaci\u00f3n de fluidos simples y complejos a escala mesosc\u00f3pica.  el problema general de los fluidos complejos, desde el punto de vista macrosc\u00f3pico de la din\u00e1mica de fluidos del continuo, es que se desconocen las ecuaciones constitutivas y se desprecia las fluctuaciones t\u00e9rmicas. desde el punto de vista microsc\u00f3pico, los pasos temporales en din\u00e1mica molecular (md) hacen inaccesible alcanzar las escalas temporales relevantes en los procesos hidrodin\u00e1micos de fluidos complejos. Por lo tanto, estos materiales requieren el uso de t\u00e9cnicas de simulaci\u00f3n y algoritmos novedosos m\u00e1s eficientes que la md, pero que resuelvan la hidrodin\u00e1mica de un fluido: son las llamadas mesosc\u00f3picas.  entre las aportaciones originales de esta tesis, destacamos las siguientes:  * hemos proporcionado a la dpd un fundamento te\u00f3rico m\u00e1s s\u00f3lido: las part\u00edculas dpd son porciones mesosc\u00f3picas del fluido que tienen una conexi\u00f3n con el fluido microsc\u00f3pico que representa. Hemos asignado una definici\u00f3n precisa del t\u00e9rmino mesoescala, conectado dos descripciones micro y mesosc\u00f3pica para el fluido, y ello que nos ha permitido comprender el origen de las fuerzas conservativas del modelo. Tambi\u00e9n hemos realizado un estudio sistem\u00e1tico de la regi\u00f3n de par\u00e1metros m\u00e1s adecuada para las simulaciones de problemas hidrodin\u00e1micos de los fluidos complejos.  * otra de las aportaciones de este trabajo es la conexi\u00f3n del modelo dpd con la t\u00e9cnica conocida como hidrodin\u00e1mica de part\u00edculas suavizadas (sph). Ello nos ha permitido generalizar la sph para aplicaciones a fluidos complejos, ya que hemos incorporado las fluctuaciones t\u00e9rmicas. En realidad el modelo dpd es una caricatura de la sph que incluye el ruido a pares. adem\u00e1s al analizar la relevancia del volumen asociado a cada part\u00edcula fluida en ambos modelos de<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Modelos para la hidrodin\u00e1mica mesosc\u00f3pica de fluidos simples y complejos<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Modelos para la hidrodin\u00e1mica mesosc\u00f3pica de fluidos simples y complejos <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Serrano Maestro M. Mar <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Nacional de educaci\u00f3n a distancia<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 16\/09\/2002<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<h3>Direcci\u00f3n y tribunal<\/h3>\n<ul>\n<li><strong>Director de la tesis<\/strong>\n<ul>\n<li>Pep Espa\u00f1ol Garrig\u00f3s<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: joaqu\u00edn Marro borau <\/li>\n<li>david Jou mirabent (vocal)<\/li>\n<li>Manuel Laso carbajo (vocal)<\/li>\n<li>raul Toral garces (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Serrano Maestro M. Mar El objetivo principal de esta tesis doctoral es la fundamentaci\u00f3n de t\u00e9cnicas de [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""}},"footnotes":""},"categories":[199,202,201,17070],"tags":[47591,20071,36644,58532,4056,58531],"class_list":["post-18969","post","type-post","status-publish","format-standard","hentry","category-fisica","category-mecanica","category-mecanica-estadistica","category-nacional-de-educacion-a-distancia","tag-david-jou-mirabent","tag-joaquin-marro-borau","tag-manuel-laso-carbajo","tag-pep-espanol-garrigos","tag-raul-toral-garces","tag-serrano-maestro-m-mar"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/18969","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/comments?post=18969"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/18969\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=18969"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=18969"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=18969"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}