{"id":11217,"date":"2001-08-06T00:00:00","date_gmt":"2001-08-06T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/estudio-de-la-turbulencia-producida-por-el-gradiente-de-temperatura-ionica-en-un-plasma-de-fusion\/"},"modified":"2001-08-06T00:00:00","modified_gmt":"2001-08-06T00:00:00","slug":"estudio-de-la-turbulencia-producida-por-el-gradiente-de-temperatura-ionica-en-un-plasma-de-fusion","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/estudio-de-la-turbulencia-producida-por-el-gradiente-de-temperatura-ionica-en-un-plasma-de-fusion\/","title":{"rendered":"Estudio de la turbulencia producida por el gradiente de temperatura i\u00f3nica en un plasma de fusi\u00f3n"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Juan  Diego Alvarez Roman <\/strong><\/h2>\n<p>El cap\u00edtulo 1 es introductorio al tema que en la memoria se desarrolla. situamos el problema de la turbulencia itg en el contexto apropiado y motivamos su estudio.  en el capitulo 2 establecemos las ecuaciones de fluido para el estudio de la turbulencia itg en geometr\u00eda cil\u00edndrica, incluyendo un t\u00e9rmino que modela el mecanismo de amortiguamiento de landau.  en el capitulo 3 realizamos un detallado an\u00e1lisis linea de las ecuaciones establecidas en el cap\u00edtulo 2, an\u00e1lisis previo necesario, que nos sirve para comprender los fen\u00f3menos no lineales.  en el cap\u00edtulo 4 hacemos una descripaci\u00f3n del m\u00e9todo num\u00e9rico empleado para la resoluci\u00f3n de las ecuaciones itg no lineales. Exponemos tambi\u00e9n su paralelizaci\u00f3n, es decir, como se desarrolla dicho m\u00e9todo num\u00e9rico en un ordenador paralelo.  en el cap\u00edtulo 5 realizamos un exhaustivo estudio de las caracter\u00edsticas de las soluciones no lineales de las ecuaciones itg y de este modo caracterizamos en gran medida la turbulencia, as\u00ed como las car\u00e1cter\u00edsticas m\u00e1s importantes asociadas al transporte.  en el cap\u00edtulo 6 hacemos un an\u00e1lisis de la respuesta adiab\u00e1tica de los electrones y vemos que la relajaci\u00f3n de la aproximaci\u00f3n de respuesta adiab\u00e1tica de los electrones da lugar a fen\u00f3menos novedosos de los que las ecuaciones itg usuales no dan cuenta.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Estudio de la turbulencia producida por el gradiente de temperatura i\u00f3nica en un plasma de fusi\u00f3n<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Estudio de la turbulencia producida por el gradiente de temperatura i\u00f3nica en un plasma de fusi\u00f3n <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Juan  Diego Alvarez Roman <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Carlos III de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 08\/06\/2001<\/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>Luis Garc\u00eda Gonzalo<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: alberto Ibort latre <\/li>\n<li>boudewijn Van milligen (vocal)<\/li>\n<li>Carlos Hidalgo vera (vocal)<\/li>\n<li> Mart\u00edn sol\u00eds Jos\u00e9 ram\u00f3n (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Juan Diego Alvarez Roman El cap\u00edtulo 1 es introductorio al tema que en la memoria se desarrolla. [&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":[18550,199,200,10842],"tags":[6173,36877,22765,36876,10573,36878],"class_list":["post-11217","post","type-post","status-publish","format-standard","hentry","category-carlos-iii-de-madrid","category-fisica","category-fisica-de-fluidos","category-fisica-de-plasmas","tag-alberto-ibort-latre","tag-boudewijn-van-milligen","tag-carlos-hidalgo-vera","tag-juan-diego-alvarez-roman","tag-luis-garcia-gonzalo","tag-martin-solis-jose-ramon"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/11217","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=11217"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/11217\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=11217"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=11217"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=11217"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}