{"id":47424,"date":"2020-04-19T13:24:00","date_gmt":"2020-04-19T13:24:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/detonaciones-confinadas-con-simetria-esferica-y-cilindrica\/"},"modified":"2020-04-19T13:24:00","modified_gmt":"2020-04-19T13:24:00","slug":"detonaciones-confinadas-con-simetria-esferica-y-cilindrica","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/detonaciones-confinadas-con-simetria-esferica-y-cilindrica\/","title":{"rendered":"Detonaciones confinadas con simetria esferica y cilindrica"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Antonio Lecuona Neumann <\/strong><\/h2>\n<p>Se describe el campo fluidodinamico generado por una detonacion iniciada en la superficie exterior de una bola o cilindro cuando esta rodeada de una cascara dematerial denso que actua de reflector. En una primera parte  para resolver las ecuaciones del movimiento fluido resultante se usan desarrollos asintoticos validos para tiempos peque\u00f1os comparados con el que tarda en llegar la detonacion al centro. El campo fluido queda comprendido entre la onda de detonacion y la onda de choque intensa generada en el reflector.  para conseguir describir la propagacion para instantes posteriores  se usa el metodo de las caracteristicas resolviendo las ecuaciones de forma aproximada.  se usan isentropicas del tipo correspondiente a un gas perfecto para el medio detonado y para el medio inerte en el caso de que se trate inicialmente de un gas. Para reflectores inicialmente liquidos o solidos se usan las ecuaciones apropiadas  obtenidas de forma experimental.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Detonaciones confinadas con simetria esferica y cilindrica<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Detonaciones confinadas con simetria esferica y cilindrica <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Antonio Lecuona Neumann <\/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\/1980<\/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>Amable Li\u00f1an Martinez<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jose Sanmartin Losada <\/li>\n<li>Antonio Crespo Martinez (vocal)<\/li>\n<li>Emilio Varela Arroyo (vocal)<\/li>\n<li>Pedro Perez Del Notario Martinez Mara\u00f1on (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Antonio Lecuona Neumann Se describe el campo fluidodinamico generado por una detonacion iniciada en la superficie exterior [&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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