{"id":2373,"date":"1994-01-01T00:00:00","date_gmt":"1994-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/1994\/01\/01\/el-medio-interestelar-local\/"},"modified":"1994-01-01T00:00:00","modified_gmt":"1994-01-01T00:00:00","slug":"el-medio-interestelar-local","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/astronomia-y-astrofisica\/el-medio-interestelar-local\/","title":{"rendered":"El medio interestelar local"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Ricardo Genova Galvan <\/strong><\/h2>\n<p>Esta disertacion se divide en dos partes, claramente diferenciadas. Una primera parte, bibliografica, comprende los capitulos primero y segundo. La segunda parte -los capitulos tercero, cuarto y quinto -resume el trabajo de investigacion. Tres apendices complementan lo expuesto en la segunda parte de la tesis.  en el capitulo primero, se resume lo que hoy conocemos sobre el medio interestelar. Se explica la morfolog\u00eda del gas que ocupa la vecindad solar, se describe este ultimo volumen, y se explican los modelos que tratan de explicar lo que en el se observa.  el gas interestelar mas proximo al sol se describe en el capitulo segundo. Se explican las interacciones entre el sol y el gas que lo circunda, se describen las tecnicas que permiten detectar el gas interestelar cuando penetra en la heliosfera, y se explican las caracteristicas del gas, segun lo que ponen de manifiesto esas observaciones.  el capitulo tercero, presenta los resultados de un programa, dedicado a explorar el gas del medio interestelar local, mediante la observacion de absorciones interestelares de mgii, en los espectros de estrellas tardias, situadas en las proximidades del sol.  la cinematica del gas local se estudia en el capitulo cuarto. En el, se ha hecho una recopilacion de las observaciones de absorciones, producidas por el gas interestelar, en las visuales dirigidas hacia las estrellas mas proximas al sol.  utilizando los metodos que se describen en los apendices, se identifican las velocidades vectoriales del gas local.  la progresiva aproximacion al sol, que se ha hecho en los capitulos precedentes, culmina en el capitulo quinto, con el estudio de lo que se ha venido a denominar nube local. En este capitulo, se utiliza todo lo que se ha expuesto en el resto de la tesis, para explicar como penetra el gas local en la heliosfera, y para discernir, a partir de la identificacion de la velocidad vectorial de dicho gas, la morfolog\u00eda del gas en las i<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>El medio interestelar local<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 El medio interestelar local <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Ricardo Genova Galvan <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 La laguna<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1994<\/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> Beckman Abramson Juan  Esteban<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Francisco Sanchez Martinez <\/li>\n<li>Ram\u00f3n Canal Masgoret (vocal)<\/li>\n<li>Rodney Davies (vocal)<\/li>\n<li>Guillermo Tenorio-tagle (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Ricardo Genova Galvan Esta disertacion se divide en dos partes, claramente diferenciadas. Una primera parte, bibliografica, comprende [&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":[7616,1050,1052,7615,9915],"tags":[10113,7770,10116,10114,10112,10115],"class_list":["post-2373","post","type-post","status-publish","format-standard","hentry","category-astronomia-optica","category-astronomia-y-astrofisica","category-cosmologia-y-cosmogonia","category-espectroscopia-astrofisica","category-la-laguna","tag-beckman-abramson-juan-esteban","tag-francisco-sanchez-Martinez","tag-guillermo-tenorio-tagle","tag-ramon-canal-masgoret","tag-ricardo-genova-galvan","tag-rodney-davies"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/2373","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=2373"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/2373\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=2373"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=2373"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=2373"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}