{"id":19312,"date":"2002-02-10T00:00:00","date_gmt":"2002-02-10T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/propiedades-termodinamicas-de-las-mezclas-hidrocarburo-eter\/"},"modified":"2002-02-10T00:00:00","modified_gmt":"2002-02-10T00:00:00","slug":"propiedades-termodinamicas-de-las-mezclas-hidrocarburo-eter","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/propiedades-termodinamicas-de-las-mezclas-hidrocarburo-eter\/","title":{"rendered":"Propiedades termodin\u00e1micas de las mezclas hidrocarburo &#8211; \u00e9ter"},"content":{"rendered":"<h2>Tesis doctoral de <strong>  R\u00edo Hern\u00e1ndez Armando Emeterio Del <\/strong><\/h2>\n<p>En este trabajo se estudian los datos de equilibrio l\u00edquido-vapor (elv) y otras propiedades de exceso de sistemas binarios formados por un hidrocarburo y un \u00e9ter ramificado. Para las medidas de equilibrio l\u00edquido-vapor de los sistemas metil tert butil \u00e9ter (mtbe) + ciclohexano, o decano; tert amil metil \u00e9ter (tame) + ciclohexano, o hexano, u octano en un intervalo de temperaturas entre 298.15 y 328.15 k y etil tert butil \u00e9ter (etbe) + ciclohexano, o hexano, o heptano desde 298.15 hasta 363.15 k se utiliz\u00f3 un aparato basado en el esquema de gibbs-van ness. Para los sistemas que contienen etbe, los datos de entalp\u00eda de exceso (hm e) fueron medidos en el intervalo de temperaturas de 313.15 hasta 393.15 k, por medio de un calor\u00edmetro isotermo de flujo.  los valores de elv se analizaron usando una modificaci\u00f3n del m\u00e9todo de barker y el principio de m\u00e1xima verosimilitud. La energ\u00eda gibbs de exceso de la fase l\u00edquida es descrita por un aproximante de pad\u00e9 en los sistemas que contienen mtbe y tame y por la ecuaci\u00f3n polin\u00f3mica de legendre en aquellos en los que el \u00e9ter es el etbe.  todos los sistemas mostraron desviaciones positivas de la ley de raoult. los datos de elv y hm e se analizaron conjuntamente con los datos de elv, hm e y vm e medidos anteriormente para estas mezclas por otros autores. los modelos uniquac, de red de s\u00e1nchez y lacombe (lf) y flory se han utilizado para correlacionar simult\u00e1neamente los datos de elv y hm e. Los dos \u00faltimos modelos se usaron adem\u00e1s para predecir los datos de vm e.  las tres versiones del modelo unifac: unifac original, unifac modificado de lyngby y unifac modificado de dortmund se han empleado para la predicci\u00f3n de los datos de elv. Adem\u00e1s, en los sistemas que contienen mtbe, los datos de elv han sido analizados con el modelo conductor like screening model (cosmo).<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Propiedades termodin\u00e1micas de las mezclas hidrocarburo &#8211; \u00e9ter<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Propiedades termodin\u00e1micas de las mezclas hidrocarburo &#8211; \u00e9ter <\/li>\n<li><strong>Autor:<\/strong>\u00a0  R\u00edo Hern\u00e1ndez Armando Emeterio Del <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Complutense de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 02\/10\/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> Rodr\u00edguez Renuncio Juan  Antonio<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: crist\u00f3bal Fern\u00e1ndez pineda <\/li>\n<li>Jos\u00e9 s. Urieta navarro (vocal)<\/li>\n<li>Jos\u00e9 Mar\u00eda Leal villalba (vocal)<\/li>\n<li>Carlos Casanova roque (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de R\u00edo Hern\u00e1ndez Armando Emeterio Del En este trabajo se estudian los datos de equilibrio l\u00edquido-vapor (elv) y [&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":[1],"tags":[3145,6651,41375,41899,59390,20604],"class_list":["post-19312","post","type-post","status-publish","format-standard","hentry","category-sin-categoria","tag-carlos-casanova-roque","tag-cristobal-fernandez-pineda","tag-jose-maria-leal-villalba","tag-jose-s-urieta-navarro","tag-rio-hernandez-armando-emeterio-del","tag-rodriguez-renuncio-juan-antonio"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/19312","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=19312"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/19312\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=19312"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=19312"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=19312"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}