{"id":104,"date":"2012-12-17T17:37:02","date_gmt":"2012-12-17T22:37:02","guid":{"rendered":"http:\/\/www.electropol.com.co\/blog\/?p=104"},"modified":"2016-06-30T15:36:42","modified_gmt":"2016-06-30T20:36:42","slug":"energia-especifica","status":"publish","type":"post","link":"https:\/\/electropol.com.co\/blog\/energia-especifica\/","title":{"rendered":"Energ\u00eda Espec\u00edfica"},"content":{"rendered":"<p>La energ\u00eda espec\u00edfica W\/R de una corriente de impulso es la energ\u00eda generada por la corriente de impulso en una resistencia de 1 \u03a9. Esta generaci\u00f3n de energ\u00eda es la integral del cuadrado de la corriente de impulso por el tiempo de duraci\u00f3n de la misma:<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Formularw.jpg\" alt=\"Formularw\" \/><\/p>\n<p><!--more--><\/p>\n<p>Por eso, la energ\u00eda espec\u00edfica se denomina, con frecuencia, como impulso del cuadrado de la corriente. Es determinante para el calentamiento de conductores por los que fluye la corriente de impulso de rayo, as\u00ed como para los efectos mec\u00e1nicos de las fuerzas magn\u00e9ticas entre conductores recorridos por corriente de impulso de rayo (Ver Figura).<\/p>\n<p>Para la energ\u00eda generada W en un conductor con la resistencia R tenemos:<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Formulaw.jpg\" alt=\"Formulaw\" \/><\/p>\n<p>Siendo:<\/p>\n<p style=\"padding-left: 30px;\"><strong>R:<\/strong> Resistencia d.c. del conductor (dependiente de la temperatura)<br \/>\n<strong>W\/R:<\/strong> Energ\u00eda espec\u00edfica<\/p>\n<p>El c\u00e1lculo del calentamiento de conductores atravesados por corriente de impulso de rayo puede resultar necesario cuando, al efectuar la planificaci\u00f3n y construcci\u00f3n de sistemas de protecci\u00f3n contra rayos, haya que tener en consideraci\u00f3n los riesgos en cuanto a la protecci\u00f3n de personas, riesgos contra incendios y riesgos de explosi\u00f3n.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Calentamiento.jpg\" alt=\"Calentamiento\" \/><\/p>\n<p>Al efectuar el c\u00e1lculo hay que partir del supuesto de que la totalidad de la energ\u00eda t\u00e9rmica es generada por la resistencia \u00f3hmica de los componentes del sistema de protecci\u00f3n contra rayos. Asimismo hay que tener en cuenta que, debido a la brevedad del proceso, no tiene lugar ning\u00fan intercambio t\u00e9rmico perceptible con el entorno. En la siguiente tabla se exponen las elevaciones de temperatura de diferentes materiales utilizados en los sistemas de protecci\u00f3n contra rayos, y sus secciones en funci\u00f3n de la energ\u00eda espec\u00edfica.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Elevacion_temperatura.jpg\" alt=\"Elevacion_temperatura\" \/><\/p>\n<p>Las fuerzas electrodin\u00e1micas F originadas por una corriente i que circula por un conductor de longitud l formado por dos ramas largas en paralelo y separadas por una distancia d (Ver Figura) pueden calcularse aproximadamente con la ecuaci\u00f3n siguiente:<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Formulaft.jpg\" alt=\"Formulaft\" \/><\/p>\n<p>Siendo:<\/p>\n<p style=\"padding-left: 30px;\"><strong>F(t):<\/strong> Fuerza electrodin\u00e1mica<br \/>\n<strong>I:<\/strong> Corriente<br \/>\n<strong>\u00b50:<\/strong> Permeabilidad magn\u00e9tica en aire (4 \u03c0\u22c510-7 H\/m)<br \/>\n<strong>l:<\/strong> Longitud de conductor<br \/>\n<strong>D:<\/strong> Distancia entre conductores en paralelo<\/p>\n<p>La acci\u00f3n de la fuerza sobre los dos conductores es de atracci\u00f3n si las dos corrientes fluyen en la misma direcci\u00f3n y es de separaci\u00f3n en el caso de sentido opuesto de las corrientes. Es proporcional al producto de las corrientes en los conductores e inversamente proporcional a la distancia existente entre los mismos.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/www.electropol.com.co\/blog\/wp-content\/uploads\/2012\/12\/Esfuerzo_fuerzas_eletromagneticas.jpg\" alt=\"Esfuerzo_fuerzas_eletromagneticas\" \/><\/p>\n<p>Pero tambi\u00e9n en el caso de un solo conductor, doblado, se produce un efecto de la fuerza sobre el conductor. En este supuesto, la fuerza es proporcional al cuadrado de la corriente en el conductor doblado.<\/p>\n<p>La energ\u00eda espec\u00edfica de la corriente de impulso determina, de este modo, el esfuerzo que causa una deformaci\u00f3n reversible o irreversible de los componentes y de la disposici\u00f3n de los mismos en un sistema de protecci\u00f3n contra rayos.<\/p>\n<p>Estos efectos son tomados en consideraci\u00f3n en los protocolos de prueba de las normas de producto referidas a las exigencias que se plantean a los componentes de uni\u00f3n para sistemas de protecci\u00f3n contra rayos.<\/p>\n<p>Si desea m\u00e1s informaci\u00f3n puede descargar: <a href=\"http:\/\/www.electropol.com.co\/blog\/blitzplaner\">BLITZPLANER &#8211; Manual de Protecci\u00f3n contra Rayos<\/a><\/p>\n<!-- AddThis Advanced Settings generic via filter on the_content --><!-- AddThis Share Buttons generic via filter on the_content -->","protected":false},"excerpt":{"rendered":"<p>La energ\u00eda espec\u00edfica W\/R de una corriente de impulso es la energ\u00eda generada por la corriente de impulso en una resistencia de 1 \u03a9. Esta generaci\u00f3n de energ\u00eda es la integral del cuadrado de la corriente de impulso por el tiempo de duraci\u00f3n de la misma:<!-- AddThis Advanced Settings generic via filter on get_the_excerpt --><!-- AddThis Share Buttons generic via filter on get_the_excerpt --><\/p>\n","protected":false},"author":10,"featured_media":110,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[18,2,17],"tags":[23],"class_list":["post-104","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-proteccion-datos","category-proteccion-externa","category-proteccion-interna","tag-energia-especifica"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.3 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Energ\u00eda Espec\u00edfica - Rayo-Resistente. Electropol Colombia Distribuidor de Weidm\u00fcller<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/electropol.com.co\/blog\/energia-especifica\/\" \/>\n<meta property=\"og:locale\" content=\"es_ES\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Energ\u00eda Espec\u00edfica - Rayo-Resistente. Electropol Colombia Distribuidor de Weidm\u00fcller\" \/>\n<meta property=\"og:description\" content=\"La energ\u00eda espec\u00edfica W\/R de una corriente de impulso es la energ\u00eda generada por la corriente de impulso en una resistencia de 1 \u03a9. 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