{"id":43963,"date":"2018-08-13T00:46:58","date_gmt":"2018-08-13T00:46:58","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/influencia-de-los-parametros-del-laser-sobre-la-hidrodinamica-de-plasmas-para-microfusion\/"},"modified":"2018-08-13T00:46:58","modified_gmt":"2018-08-13T00:46:58","slug":"influencia-de-los-parametros-del-laser-sobre-la-hidrodinamica-de-plasmas-para-microfusion","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/influencia-de-los-parametros-del-laser-sobre-la-hidrodinamica-de-plasmas-para-microfusion\/","title":{"rendered":"Influencia de los parametros del laser sobre la hidrodinamica de plasmas para microfusion."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Antonio Barrero Ripoll <\/strong><\/h2>\n<p>En el presente trabajo se ha considerado el movimiento cuasineutro  unidimensional de un plasma infinito  frio y de densidad uniforme  generado por la absorcion en un plano dado  de un pulso lineal de energia por unidad de area y tiempo  el analisis incluye conduccion termica y viscosidad de iones y electrones  intercambio energetico entre ambas especies y limitador de flujo termico electronico. Se encuentra que las ecuaciones que gobiernan el movimiento admiten solucion de semejanza y que el caracter del movimiento depende de un unico parametro adimensional. Se ha obtenido el comportamiento asintotico de la solucion de dichas ecuaciones discutiendose tambien el comportamiento de la solucion.  el analisis se puede extender facilmente al caso de un plasma que inicialmente ocupa un semiespacio y proporciona informacion sobre la hidrodinamica del proceso de la fusion con laser.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Influencia de los parametros del laser sobre la hidrodinamica de plasmas para microfusion.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Influencia de los parametros del laser sobre la hidrodinamica de plasmas para microfusion. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Antonio Barrero Ripoll <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Polit\u00e9cnica de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1977<\/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>Juan  Ramon Sanmart\u00edn Losada<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Carlos Sanchez Tarifa <\/li>\n<li>Amable Li\u00f1an Martinez (vocal)<\/li>\n<li> Da Riva De La Cavada Ignacio (vocal)<\/li>\n<li>Guillermo Velarde Pinacho (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Antonio Barrero Ripoll En el presente trabajo se ha considerado el movimiento cuasineutro unidimensional de un plasma [&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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