{"id":89208,"date":"2001-08-03T00:00:00","date_gmt":"2001-08-03T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/estudio-experimental-de-la-propagacion-de-una-llama-sobre-combustible-la%c2%adquido\/"},"modified":"2001-08-03T00:00:00","modified_gmt":"2001-08-03T00:00:00","slug":"estudio-experimental-de-la-propagacion-de-una-llama-sobre-combustible-la%c2%adquido","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/estudio-experimental-de-la-propagacion-de-una-llama-sobre-combustible-la%c2%adquido\/","title":{"rendered":"Estudio experimental de la propagaci\u00f3n de una llama sobre combustible l\u00edquido"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Eugenio Degroote Herranz <\/strong><\/h2>\n<p>El estudio experimental de la propagaci\u00f3n de una llama sobre combustibles l\u00edquido ha sido realizado en una serie de canales rectangulares de dimensiones variables. La representaci\u00f3n de la velocidad avance de la llama (vf) en funci\u00f3n de la temperatura suprficial inicial del l\u00edquido, ha revelado la existencia de cinco reg\u00edmenes distintos de avance de la llama, que han sido debidamente caracterizados. Asimismo, las cuatro temperaturas de transici\u00f3n observadas han sido estudiadas. Para temperaturas intermedias, se observa un avance oscilante de la llama, mientras que, para el resto de las temperaturas, el avance es (con caracter\u00edsticas diferenciadas en cada caso) uniforme. se han puesto asimismo en evidencia los mecanismos que controlan el avance de la llama, resultando que, para temperaturas altas, el avance de la llama es an\u00e1logo al de un s\u00f3lido. Mientras que, para temperaturas menores a una temperatura cr\u00edtica tfd, se observa la aparici\u00f3n de una zona de convecci\u00f3n termocapilar delante de la llama, que modifica el modo de propagaci\u00f3n de \u00e9sta. Este efecto de asistencia a trav\u00e9s de la fase l\u00edquida produce los distintos modos de propagaci\u00f3n observados, y resulta ser el responsable del comportamiento oscilante de la llama, cuyo mecanismo es asimismo explicado de forma cualitativa.  distintas consideraciones nos llevan a definir el par\u00e1metro adimensional s=us\/vf, siendo us la velocidad caracter\u00edstica del l\u00edquido en el borde de la llama, el an\u00e1lisis estad\u00edstico de los datos experimentales indica que, para la tempertura de transici\u00f3n tfd, s es pr\u00e1cticamente utilizados, siendo muy pr\u00f3ximo a 1.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Estudio experimental de la propagaci\u00f3n de una llama sobre combustible l\u00edquido<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Estudio experimental de la propagaci\u00f3n de una llama sobre combustible l\u00edquido <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Eugenio Degroote Herranz <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Nacional de educaci\u00f3n a distancia<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 08\/03\/2001<\/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>Pedro Luis Garc\u00eda Ybarra<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jos\u00e9 Carlos Antoranz callejo <\/li>\n<li> Higuera ant\u00f3n Francisco j. (vocal)<\/li>\n<li>rosa Mar\u00eda Benito zafrilla (vocal)<\/li>\n<li>Antonio Lozano fantoba (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Eugenio Degroote Herranz El estudio experimental de la propagaci\u00f3n de una llama sobre combustibles l\u00edquido ha sido [&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":[199,200,21211,1192,17070,560],"tags":[63498,131932,107214,31596,54013,30142],"class_list":["post-89208","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-de-fluidos","category-llamas","category-mecanica-de-fluidos","category-nacional-de-educacion-a-distancia","category-quimica-fisica","tag-antonio-lozano-fantoba","tag-eugenio-degroote-herranz","tag-higuera-anton-francisco-j","tag-jose-carlos-antoranz-callejo","tag-pedro-luis-garcia-ybarra","tag-rosa-maria-benito-zafrilla"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/89208","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=89208"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/89208\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=89208"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=89208"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=89208"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}