{"id":135308,"date":"1997-01-01T00:00:00","date_gmt":"1997-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/efectos-de-tamano-finito-en-sistemas-de-particulas-duras\/"},"modified":"1997-01-01T00:00:00","modified_gmt":"1997-01-01T00:00:00","slug":"efectos-de-tamano-finito-en-sistemas-de-particulas-duras","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/efectos-de-tamano-finito-en-sistemas-de-particulas-duras\/","title":{"rendered":"Efectos de tama\u00f1o finito en sistemas de particulas duras."},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Roman Hernandez Francisco Lorenzo <\/strong><\/h2>\n<p>En este trabajo se han estudiado los efectos de tama\u00f1o finito que aparecen al considerar un sistema con un numero finito de particulas duras. En particular, se ha realizado un estudio de las distribuciones de momento en el marco de la colectividad microcanonica (efectos explicitos), y de la colectividad microcanonica con conservacion de momento lineal total (efectos implicitos). Tambien se ha realizado un estudio de las distribuciones de momento en el caso de que los sistemas se encuentren en presencia de un campo externo. En todos los casos se han analizado las discrepancias con respecto a la distribucion de maxwell boltzmann. Por otra parte, a partir de la conexion existente entre la funcion de distribucion radial y la fluctuacion relativa, se han estudiado los efectos explicitos de tama\u00f1o finito que afectan en el calculo de las fluctuaciones en el numero de particulas sobre un subvolumen en un fluido de discos duros en equilibrio. Por ultimo se han estudiado los efectos de tama\u00f1o finito que aparecen en las fluctuaciones relativas en el problema de la absorcion secuencial aleatoria.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Efectos de tama\u00f1o finito en sistemas de particulas duras.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Efectos de tama\u00f1o finito en sistemas de particulas duras. <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Roman Hernandez Francisco Lorenzo <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Salamanca<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1997<\/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>Santiago Velasco Maillo<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Cristobal Fernandez Pineda <\/li>\n<li>Julio Guemez Ledesma (vocal)<\/li>\n<li>Carlos Santamaria Salazar (vocal)<\/li>\n<li> Iglesias Perez Fco. Javier (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Roman Hernandez Francisco Lorenzo En este trabajo se han estudiado los efectos de tama\u00f1o finito que aparecen [&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":[199,202,201,9386],"tags":[9687,6651,249511,9757,249510,9756],"class_list":["post-135308","post","type-post","status-publish","format-standard","hentry","category-fisica","category-mecanica","category-mecanica-estadistica","category-salamanca","tag-carlos-santamaria-salazar","tag-cristobal-fernandez-pineda","tag-iglesias-perez-fco-javier","tag-julio-guemez-ledesma","tag-roman-hernandez-francisco-lorenzo","tag-santiago-velasco-maillo"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/135308","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=135308"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/135308\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=135308"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=135308"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=135308"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}