{"id":139694,"date":"2026-01-12T17:47:56","date_gmt":"2026-01-12T17:47:56","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/estudio-de-los-nitratos-alcalinos-xno3-xli-na-k-cs-por-calorimetria-diferencial-de-barrido-d-s-c-determinacion-de-las-funciones-de-exceso\/"},"modified":"2026-01-12T17:47:56","modified_gmt":"2026-01-12T17:47:56","slug":"estudio-de-los-nitratos-alcalinos-xno3-xli-na-k-cs-por-calorimetria-diferencial-de-barrido-d-s-c-determinacion-de-las-funciones-de-exceso","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/estudio-de-los-nitratos-alcalinos-xno3-xli-na-k-cs-por-calorimetria-diferencial-de-barrido-d-s-c-determinacion-de-las-funciones-de-exceso\/","title":{"rendered":"Estudio de los nitratos alcalinos xno3, (x=li, na, k, cs), por calorimetria diferencial de barrido (d.s.c.). determinacion de las funciones de exceso."},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Maeso Marcos M. Jes\u00fas <\/strong><\/h2>\n<p>Se ha puesto a punto la metodolog\u00eda de la tecnica d.S.C.  en la determinacion de las magnitudes temperatura y entalpia de fusion y de transicion, en su caso, para los cristales x no3 (x=li, na, k y cs). Se determina el calor especifico en funcion de la temperatura para cada uno de los nitratos puros en el rango 350-700 k, calculandose ademas su variacion en la fusion. Se evaluan las funciones termodinamicas estandar. Se construyen los diagramas de fase solido-liquido de las mezclas binarias (li-na)no3, (li-k)no3 y (na-k)no3. Se determinan para los tres sistemas binarios unos potenciales promedio de interaccion. A partir del estudio del potencial de gibbs de exceso, a composicion equimolecular, para las mezclas binarias contrastando con los del calor de mezcla, se obtiene evidencia del comportamiento regular de las mismas. Se determinan los coeficientes de actividad de cada nitrato en la respectiva mezcla liquida y a partir de ellos el potencial de gibbs de exceso para la mezcla en funcion de la composicion molar.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Estudio de los nitratos alcalinos xno3, (x=li, na, k, cs), por calorimetria diferencial de barrido (d.s.c.). determinacion de las funciones de exceso.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Estudio de los nitratos alcalinos xno3, (x=li, na, k, cs), por calorimetria diferencial de barrido (d.s.c.). determinacion de las funciones de exceso. <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Maeso Marcos M. Jes\u00fas <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Cantabria<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1992<\/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>Julio Largo Cabrerizo<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jaime Amor\u00f3s Arnau <\/li>\n<li> Villama\u00f1an Olfos Miguel Angel (vocal)<\/li>\n<li>Carlos Casanova Roque (vocal)<\/li>\n<li> Rodriguez Gonzalez Julio Ramon (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Maeso Marcos M. Jes\u00fas Se ha puesto a punto la metodolog\u00eda de la tecnica d.S.C. en la [&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":[7477,10518,199,20151,560,2793],"tags":[3145,10602,111750,254219,40387,12848],"class_list":["post-139694","post","type-post","status-publish","format-standard","hentry","category-cambio-de-fase","category-cantabria","category-fisica","category-fisica-del-estado-liquido","category-quimica-fisica","category-termodinamica","tag-carlos-casanova-roque","tag-jaime-amoros-arnau","tag-julio-largo-cabrerizo","tag-maeso-marcos-m-jesus","tag-rodriguez-gonzalez-julio-ramon","tag-villamanan-olfos-miguel-angel"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/139694","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=139694"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/139694\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=139694"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=139694"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=139694"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}