{"id":18999,"date":"2018-03-09T09:07:49","date_gmt":"2018-03-09T09:07:49","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/presiones-de-vapor-y-gme-de-mezclas-binarias-no-electrola%c2%adticas-conteniendo-un-alcohol-estudio-termodinamico\/"},"modified":"2018-03-09T09:07:49","modified_gmt":"2018-03-09T09:07:49","slug":"presiones-de-vapor-y-gme-de-mezclas-binarias-no-electrola%c2%adticas-conteniendo-un-alcohol-estudio-termodinamico","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/presiones-de-vapor-y-gme-de-mezclas-binarias-no-electrola%c2%adticas-conteniendo-un-alcohol-estudio-termodinamico\/","title":{"rendered":"Presiones de vapor y gme de mezclas binarias no-electrol\u00edticas conteniendo un alcohol: estudio termodin\u00e1mico"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Santiago Mart\u00ednez Masip <\/strong><\/h2>\n<p>Se han medido las presiones de saturaci\u00f3n de mezclas de 1-clorobutano, 0 1-bromobutano con alcoholes lineales de 2,4,6,8 y 10 \u00e1tomos de carbono de longitud as\u00ed como los cuatro is\u00f3meros del butanol en todo el rango de fracciones molares a intervalos de cinco grados entre 278.15 k y 323.15 k, por un m\u00e9todo est\u00e1tico excepto para los sistemas con ter-butanol (desde 298.15 k hasta 323.15k) y 1-decanol (desde 283.15k hasta 323.15k). Tambi\u00e9n se han medido entalp\u00edas y vol\u00famenes de exceso, a 298.15k, de 1-clorobutano con 2-butanol o iso-butanol y de 1-bromobutano con los is\u00f3meros del butanol o 1-octanol).  la reducci\u00f3n de datos de presi\u00f3n de vapor (p,x,t) para obtener coeficientes de actividad y gme se ha llevado a cabo seg\u00fan el m\u00e9todo de barker. Para determinar la consistencia de los datos de presi\u00f3n de vapor, se ha aplicado la relaci\u00f3n de gibbs-helmholtz, observando, en general, un buen acuerdo con los datos experimental de hme.  en aquellos sistemas que presentan azeotrop\u00eda, se han calculado las coordenadas azeotr\u00f3picas (z,pz). La composici\u00f3n azeotr\u00f3pica muestra una buena correlaci\u00f3n lineal frente a t, y ln pz frente a 1\/t.  se ha utilizado el modelo eras para caracterizar las interacciones espec\u00edficas c1-oh o br-oh que se manifiestan en las mezclas estudiadas. Para ello se han determinado dos parejas -una por disolvente- de par\u00e1metros cruzados (ah*ab &#8211; av*ab), f\u00edsicamente aceptables, que mejor reproducen el comportamiento experimental de todas las mezclas estudiadas.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Presiones de vapor y gme de mezclas binarias no-electrol\u00edticas conteniendo un alcohol: estudio termodin\u00e1mico<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Presiones de vapor y gme de mezclas binarias no-electrol\u00edticas conteniendo un alcohol: estudio termodin\u00e1mico <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Santiago Mart\u00ednez Masip <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Zaragoza<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 17\/09\/2002<\/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>Pascual P\u00e9rez P\u00e9rez<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Antonio Roig muntaner <\/li>\n<li> Ureita navarro Jos\u00e9 Santiago (vocal)<\/li>\n<li>enrique Fatas lahoz (vocal)<\/li>\n<li>irene Ba\u00f1os arribas (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Santiago Mart\u00ednez Masip Se han medido las presiones de saturaci\u00f3n de mezclas de 1-clorobutano, 0 1-bromobutano con [&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":[199,2793,13610],"tags":[58598,12841,42978,58597,58596,58599],"class_list":["post-18999","post","type-post","status-publish","format-standard","hentry","category-fisica","category-termodinamica","category-zaragoza","tag-antonio-roig-muntaner","tag-enrique-fatas-lahoz","tag-irene-banos-arribas","tag-pascual-perez-perez","tag-santiago-Martinez-masip","tag-ureita-navarro-jose-santiago"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/18999","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=18999"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/18999\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=18999"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=18999"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=18999"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}