{"id":143008,"date":"1993-01-01T00:00:00","date_gmt":"1993-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/descripcion-funcional-de-haces-de-rayos-x-de-baja-energia-mediante-su-curva-de-atenuacion-en-haz-delgado\/"},"modified":"1993-01-01T00:00:00","modified_gmt":"1993-01-01T00:00:00","slug":"descripcion-funcional-de-haces-de-rayos-x-de-baja-energia-mediante-su-curva-de-atenuacion-en-haz-delgado","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/descripcion-funcional-de-haces-de-rayos-x-de-baja-energia-mediante-su-curva-de-atenuacion-en-haz-delgado\/","title":{"rendered":"Descripcion funcional de haces de rayos x de baja energia mediante su curva de atenuacion en haz delgado."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Pedro Ortiz Lopez <\/strong><\/h2>\n<p>La curva de atenuacion es la forma mas empleada de caracterizar y obtener informacion de haces de rayos x de baja energia. A partir de dicha curva se reconstruye la distribucion espectral del haz, que a su vez se utiliza para calcular magnitudes radiometricas y dosimetricas.  pero dicha reconstruccion es matematicamente inestable.  en este trabajo se plantea la alternativa de considerar la curva de atenuacion como descripcion funcional completa del haz. Asimismo se desarrolla la metodolog\u00eda para utilizarla directamente en el calculo de las mencionadas magnitudes.  se demuestra la estabilidad del metodo y se formula la ecuacion de transporte del campo de radiacion en funcion de la curva de atenuacion. Se efectua una validacion del metodo por comparacion con los resultados de otros autores, y se aplica al calculo de magnitudes concretas y a la proteccion radiologica.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Descripcion funcional de haces de rayos x de baja energia mediante su curva de atenuacion en haz delgado.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Descripcion funcional de haces de rayos x de baja energia mediante su curva de atenuacion en haz delgado. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Pedro Ortiz Lopez <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Complutense de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1993<\/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>Victor Delgado Martinez<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jose Campos Gutierrez <\/li>\n<li>Antonio Ferrer Soria (vocal)<\/li>\n<li>Eliseo Va\u00f1\u00f3 Carruana (vocal)<\/li>\n<li>Isabel Mellado Jimenez (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Pedro Ortiz Lopez La curva de atenuacion es la forma mas empleada de caracterizar y obtener informacion [&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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