{"id":140628,"date":"2026-01-12T17:56:18","date_gmt":"2026-01-12T17:56:18","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/transicion-a-la-irreversibilidad-dispersion-de-taylor-y-termodinamica-extendida\/"},"modified":"2026-01-12T17:56:18","modified_gmt":"2026-01-12T17:56:18","slug":"transicion-a-la-irreversibilidad-dispersion-de-taylor-y-termodinamica-extendida","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/transicion-a-la-irreversibilidad-dispersion-de-taylor-y-termodinamica-extendida\/","title":{"rendered":"Transicion a la irreversibilidad: dispersion de taylor y termodinamica extendida"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Juan Camacho Castro <\/strong><\/h2>\n<p>A traves del esquema de la termodinamica extendida, abordamos el estudio de la transicion de un regimen reversible a tiempos cortos a uno puramente irreversible a tiempos largos. La ecuacion que obtenemos para describir esta transicion es del tipo del telegrafista.  aplicamos este modelo general a dos sistemas macroscopicos que exhiben una transicion de este tipo: la dispersion de taylor, y la dispersion de un trazador en medios porosos.  en el primer caso, mostramos que es posible definir una entropia, un flujo y una produccion de entropia, lo cual justifica el procedimiento seguido para obtener el modelo global.  por ultimo, extendemos los resultados anteriores al contexto de las ecuaciones cineticas. Generalizamos la funcion h de boltzmann de forma que sea posible formular un teorema h para ecuaciones cineticas del telegrafista.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Transicion a la irreversibilidad: dispersion de taylor y termodinamica extendida<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Transicion a la irreversibilidad: dispersion de taylor y termodinamica extendida <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Juan Camacho Castro <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de barcelona<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1992<\/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>David Jou Mirabent<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jose Casas Vazquez <\/li>\n<li>Javier Brey Avalo (vocal)<\/li>\n<li>Lebon Georgy (vocal)<\/li>\n<li>Manuel Tello (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Juan Camacho Castro A traves del esquema de la termodinamica extendida, abordamos el estudio de la transicion [&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 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