{"id":48195,"date":"2019-11-08T14:44:21","date_gmt":"2019-11-08T13:44:21","guid":{"rendered":"https:\/\/www.thermal-engineering.org\/o-que-e-eficiencia-termica-definicao\/"},"modified":"2020-01-27T17:38:52","modified_gmt":"2020-01-27T16:38:52","slug":"o-que-e-eficiencia-termica-definicao","status":"publish","type":"post","link":"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-eficiencia-termica-definicao\/","title":{"rendered":"O que \u00e9 efici\u00eancia t\u00e9rmica &#8211; Defini\u00e7\u00e3o"},"content":{"rendered":"<div class=\"su-quote su-quote-style-default\">\n<div class=\"su-quote-inner su-clearfix\">A efici\u00eancia t\u00e9rmica, \u03b7\u00aa, de qualquer motor t\u00e9rmico \u00e9 definida como a raz\u00e3o entre o trabalho e a entrada de calor.\u00a0Para calcular a efici\u00eancia t\u00e9rmica, os engenheiros costumam usar entalpia.\u00a0Engenharia T\u00e9rmica<\/div>\n<\/div>\n<div class=\"su-divider su-divider-style-dotted\"><\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>Efici\u00eancia t\u00e9rmica<\/h2>\n<p>Um\u00a0<a title=\"Motores t\u00e9rmicos\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-o-heat-engine-definicao\/\"><strong>mecanismo t\u00e9rmico ideal<\/strong><\/a>\u00a0\u00e9 um mecanismo imagin\u00e1rio no qual a energia extra\u00edda como calor do reservat\u00f3rio de alta temperatura \u00e9 convertida completamente em funcionamento.\u00a0Mas, de acordo com a\u00a0<a title=\"Declara\u00e7\u00e3o da Segunda Lei de Kelvin-Planck\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/kelvin-planck-statement-of-the-second-law\/\"><strong>declara\u00e7\u00e3o de Kelvin-Planck<\/strong><\/a>\u00a0, esse mecanismo violaria a segunda lei da termodin\u00e2mica, porque deve haver perdas no processo de convers\u00e3o.\u00a0O calor l\u00edquido adicionado ao sistema deve ser maior que o trabalho l\u00edquido realizado pelo sistema.<\/p>\n<p><strong>Declara\u00e7\u00e3o de Kelvin-Planck:<\/strong><\/p>\n<p><em>\u201c\u00c9 imposs\u00edvel construir um dispositivo que opera em um ciclo e n\u00e3o produz outro efeito sen\u00e3o a produ\u00e7\u00e3o de trabalho e a transfer\u00eancia de calor de um \u00fanico corpo\u201d.<\/em><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>F\u00f3rmula de efici\u00eancia t\u00e9rmica<\/h2>\n<p>Como resultado de esta afirma\u00e7\u00e3o, que definem a\u00a0<strong>efici\u00eancia t\u00e9rmica<\/strong>\u00a0,\u00a0<strong><em>\u03b7\u00a0<\/em><\/strong><strong><em><sub>th<\/sub><\/em><\/strong>\u00a0, de qualquer motor de calor como a raz\u00e3o entre o\u00a0<a title=\"Trabalho em Termodin\u00e2mica\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-trabalho-em-termodinamica-definicao\/\">trabalho<\/a>\u00a0que faz,\u00a0<strong>W<\/strong>\u00a0, para o\u00a0<a title=\"Calor na Termodin\u00e2mica\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-calor-na-fisica-calor-definicao\/\">calor<\/a>\u00a0de entrada a uma temperatura elevada, Q\u00a0<sub>H<\/sub>\u00a0.<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-1.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-16945 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-1.png\" alt=\"f\u00f3rmula de efici\u00eancia t\u00e9rmica - 1\" width=\"125\" height=\"82\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-1.png\" \/><\/a><\/p>\n<p>A\u00a0<strong>efici\u00eancia t\u00e9rmica<\/strong>\u00a0,\u00a0<strong><em>\u03b7\u00a0<\/em><\/strong><strong><em><sub>th<\/sub><\/em><\/strong>\u00a0, representa a fra\u00e7\u00e3o de\u00a0<strong>calor<\/strong>\u00a0,\u00a0<strong>Q\u00a0<sub>H<\/sub><\/strong>\u00a0, que \u00e9 convertida\u00a0<strong>em trabalho<\/strong>\u00a0.\u00a0\u00c9 uma medida de desempenho adimensional de um motor t\u00e9rmico que usa energia t\u00e9rmica, como uma turbina a vapor, um motor de combust\u00e3o interna ou um refrigerador.\u00a0Para uma refrigera\u00e7\u00e3o ou bombas de calor, a efici\u00eancia t\u00e9rmica indica at\u00e9 que ponto a energia adicionada pelo trabalho \u00e9 convertida na produ\u00e7\u00e3o l\u00edquida de calor.\u00a0Como \u00e9 um n\u00famero sem dimens\u00e3o, devemos sempre expressar W, Q\u00a0<sub>H<\/sub>\u00a0e Q\u00a0<sub>C<\/sub>\u00a0nas mesmas unidades.<\/p>\n<p>Como a energia \u00e9 conservada de acordo com a\u00a0<a title=\"Primeira Lei da Termodin\u00e2mica\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-a-primeira-lei-da-termodinamica-definicao\/\"><strong>primeira lei da termodin\u00e2mica<\/strong>\u00a0<\/a>e a energia n\u00e3o pode ser convertida para funcionar completamente, a entrada de calor, Q\u00a0<sub>H<\/sub>\u00a0, deve ser igual ao trabalho realizado, W, mais o calor que deve ser dissipado como\u00a0<strong>calor residual Q\u00a0<sub>C<\/sub><\/strong>\u00a0no meio Ambiente.\u00a0Portanto, podemos reescrever a f\u00f3rmula da efici\u00eancia t\u00e9rmica como:<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-2.png\"><img loading=\"lazy\" class=\"aligncenter size-medium wp-image-16944 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-2-300x71.png\" alt=\"f\u00f3rmula de efici\u00eancia t\u00e9rmica - 2\" width=\"300\" height=\"71\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-2-300x71.png\" \/><\/a><\/p>\n<p>Para fornecer a efici\u00eancia em porcentagem, multiplicamos a f\u00f3rmula anterior por 100. Observe que\u00a0<strong><em>\u03b7\u00a0<\/em><\/strong><strong><em><sub>th<\/sub><\/em><\/strong>\u00a0pode ser 100% apenas se o calor residual Q\u00a0<sub>C<\/sub>\u00a0for zero.<\/p>\n<p>Em geral, a efici\u00eancia dos\u00a0<strong>melhores motores t\u00e9rmicos<\/strong>\u00a0\u00e9 bastante baixa.\u00a0Em suma, \u00e9\u00a0<strong>muito dif\u00edcil<\/strong>\u00a0para converter\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-energia-interna-energia-termica-definicao\/\">energia t\u00e9rmica<\/a>\u00a0a\u00a0<a title=\"O que \u00e9 energia mec\u00e2nica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/what-is-mechanical-energy\/\">energia mec\u00e2nica<\/a>\u00a0.\u00a0As efici\u00eancias t\u00e9rmicas geralmente s\u00e3o\u00a0<strong>inferiores a 50%<\/strong>\u00a0e geralmente muito abaixo.\u00a0Tenha cuidado ao compar\u00e1-lo com a efici\u00eancia da energia e\u00f3lica ou hidrel\u00e9trica (turbinas e\u00f3licas n\u00e3o s\u00e3o motores de calor), n\u00e3o h\u00e1 convers\u00e3o de energia entre a energia t\u00e9rmica e a mec\u00e2nica.<\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<h2><span>Causas de inefici\u00eancia<\/span><\/h2>\n<p><span>Como foi discutido, uma efici\u00eancia pode variar entre 0 e 1. Cada mecanismo t\u00e9rmico \u00e9 de alguma forma ineficiente.\u00a0Essa inefici\u00eancia pode ser atribu\u00edda a tr\u00eas causas.<\/span><\/p>\n<ul>\n<li><strong><span>Irreversibilidade de processos<\/span><\/strong><span>\u00a0.\u00a0Existe um limite superior te\u00f3rico geral para a efici\u00eancia da convers\u00e3o de calor em trabalho em qualquer motor t\u00e9rmico.\u00a0Esse limite superior \u00e9 chamado de\u00a0<\/span><strong><span>efici\u00eancia de Carnot<\/span><\/strong><span>\u00a0.\u00a0De acordo com o\u00a0<\/span><strong><span>princ\u00edpio Carnot<\/span><\/strong><span>\u00a0, nenhum motor pode ser mais eficiente que um motor revers\u00edvel (\u00a0<\/span><strong><span>um motor t\u00e9rmico Carnot<\/span><\/strong><span>\u00a0) operando entre os mesmos reservat\u00f3rios de alta temperatura e baixa temperatura.\u00a0Por exemplo, quando o reservat\u00f3rio quente tiver T\u00a0<\/span><sub><span>quente<\/span><\/sub><span>\u00a0de 400 \u00b0 C (673K) e T\u00a0<\/span><sub><span>frio<\/span><\/sub><span>\u00a0de cerca de 20 \u00b0 C (293K), a efici\u00eancia m\u00e1xima (ideal) ser\u00e1: = 1 &#8211; T\u00a0<\/span><sub><span>frio<\/span><\/sub><span>\u00a0\/ T\u00a0<\/span><sub><span>quente<\/span><\/sub><span>\u00a0= 1 &#8211; 293 \/ 673 = 56%.\u00a0Mas todos os processos termodin\u00e2micos reais s\u00e3o de alguma forma\u00a0<\/span><strong><span>irrevers\u00edveis<\/span><\/strong><span>.\u00a0Eles n\u00e3o s\u00e3o feitos infinitamente devagar.\u00a0Portanto, os motores t\u00e9rmicos devem ter efici\u00eancias mais baixas do que os limites de efici\u00eancia devido \u00e0 irreversibilidade inerente ao ciclo dos motores t\u00e9rmicos que utilizam.<\/span><\/li>\n<li><strong><span>Presen\u00e7a de fric\u00e7\u00e3o e perdas de calor.\u00a0<\/span><\/strong><span>Em sistemas termodin\u00e2micos reais ou em motores t\u00e9rmicos reais, uma parte da inefici\u00eancia geral do ciclo \u00e9 devida \u00e0s perdas dos componentes individuais.\u00a0Em dispositivos reais (como turbinas, bombas e compressores), um\u00a0<\/span><strong><span>atrito mec\u00e2nico<\/span><\/strong><span>\u00a0,\u00a0<\/span><strong><span>perdas de calor<\/span><\/strong><span>\u00a0e perdas no processo de combust\u00e3o causam mais perdas de efici\u00eancia.<\/span><\/li>\n<li><strong><span>Inefici\u00eancia do projeto<\/span><\/strong><span>\u00a0.\u00a0Finalmente, a \u00faltima e tamb\u00e9m importante fonte de inefici\u00eancias prov\u00e9m dos\u00a0<\/span><strong><span>compromissos<\/span><\/strong><span>\u00a0assumidos pelos\u00a0<\/span><strong><span>engenheiros<\/span><\/strong><span>\u00a0ao projetar um motor t\u00e9rmico (por exemplo, usina).\u00a0Eles devem considerar o custo e outros fatores no design e opera\u00e7\u00e3o do ciclo.\u00a0Como exemplo, considere um projeto do\u00a0<\/span><strong><span>condensador<\/span><\/strong><span>\u00a0nas usinas termel\u00e9tricas.\u00a0Idealmente, o vapor descarregado no condensador n\u00e3o teria\u00a0<\/span><strong><span>sub-resfriamento<\/span><\/strong><span>\u00a0.\u00a0Mas os condensadores reais s\u00e3o projetados para sub-resfriar o l\u00edquido em alguns graus Celsius, a fim de evitar a\u00a0<\/span><a title=\"Cavita\u00e7\u00e3o por suc\u00e7\u00e3o\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/fluid-dynamics\/centrifugal-pumps\/cavitation\/suction-cavitation\/\"><strong><span>cavita\u00e7\u00e3o de suc\u00e7\u00e3o<\/span><\/strong><\/a><span>\u00a0nas bombas de condensado.\u00a0Por\u00e9m, esse sub-resfriamento aumenta a inefici\u00eancia do ciclo, porque \u00e9 necess\u00e1ria mais energia para reaquecer a \u00e1gua.<\/span><\/li>\n<\/ul>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Efici\u00eancia t\u00e9rmica e a segunda lei<\/span><\/h2>\n<p><span>A\u00a0<\/span><a title=\"Segunda Lei da Termodin\u00e2mica\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-a-segunda-lei-da-termodinamica-definicao\/\"><strong><span>segunda lei da termodin\u00e2mica<\/span><\/strong><\/a><span>\u00a0pode ser expressa de v\u00e1rias maneiras espec\u00edficas.\u00a0Cada declara\u00e7\u00e3o expressa a mesma lei.\u00a0Listados abaixo est\u00e3o tr\u00eas que s\u00e3o frequentemente encontrados.<\/span><\/p>\n<ul>\n<li><a title=\"Clausius Declara\u00e7\u00e3o da Segunda Lei\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/clausius-statement-of-the-second-law\/\"><span>Declara\u00e7\u00e3o Clausius<\/span><\/a><\/li>\n<li><a title=\"Declara\u00e7\u00e3o da Segunda Lei de Kelvin-Planck\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/kelvin-planck-statement-of-the-second-law\/\"><span>Declara\u00e7\u00e3o de Kelvin-Planck<\/span><\/a><\/li>\n<li><a title=\"Entropia e a Segunda Lei da Termodin\u00e2mica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/entropy-and-the-second-law-of-thermodynamics\/\"><span>Entropia e a Segunda Lei<\/span><\/a><\/li>\n<\/ul>\n<p><span>Antes dessas declara\u00e7\u00f5es, devemos lembrar o trabalho de\u00a0\u00a0<\/span><strong><span>um engenheiro e f\u00edsico franc\u00eas,\u00a0<\/span><b><span>Nicolas L\u00e9onard Sadi Carnot, que\u00a0<\/span><\/b><span>avan\u00e7ou o estudo da segunda lei, formando um princ\u00edpio (\u00a0<\/span><span>tamb\u00e9m chamado\u00a0<\/span><b><span>de regra de Carnot\u00a0<\/span><\/b><span>) que especifica limites para a m\u00e1xima efici\u00eancia que qualquer motor t\u00e9rmico pode obter .<\/span><\/strong><\/p>\n<div class=\"su-spacer\"><\/div>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<h2><span>Efici\u00eancia t\u00e9rmica de motores t\u00e9rmicos<\/span><\/h2>\n<p><span>Em geral, a efici\u00eancia dos melhores motores t\u00e9rmicos \u00e9 bastante baixa.\u00a0Em resumo, \u00e9\u00a0<\/span><strong><span>muito dif\u00edcil converter energia t\u00e9rmica em energia mec\u00e2nica<\/span><\/strong><span>\u00a0.\u00a0As efici\u00eancias t\u00e9rmicas geralmente s\u00e3o inferiores a 50% e geralmente muito abaixo.<\/span><\/p>\n<figure id=\"attachment_16961\" class=\"wp-caption alignright\" aria-describedby=\"caption-attachment-16961\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-engines-turbines-min.png\"><img loading=\"lazy\" class=\"size-medium wp-image-16961 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-engines-turbines-min-300x222.png\" alt=\"Takaishi, Tatsuo;  Numata, Akira;  Nakano, Ryouji;  Sakaguchi, Katsuhiko (mar\u00e7o de 2008).\" width=\"300\" height=\"222\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-engines-turbines-min-300x222.png\" \/><\/a><figcaption id=\"caption-attachment-16961\" class=\"wp-caption-text\"><span>Takaishi, Tatsuo;\u00a0Numata, Akira;\u00a0Nakano, Ryouji;\u00a0Sakaguchi, Katsuhiko (mar\u00e7o de 2008).\u00a0\u201cAbordagem para motores a diesel e g\u00e1s de alta efici\u00eancia\u201d (PDF).\u00a0Revis\u00e3o t\u00e9cnica Mitsubishi Heavy Industries.\u00a045 (1).\u00a0P\u00e1gina visitada em 2011-02-04.<\/span><\/figcaption><\/figure>\n<p><span>\u00c9 f\u00e1cil produzir energia t\u00e9rmica fazendo o trabalho, por exemplo, por qualquer processo de atrito.\u00a0Mas conseguir trabalho com energia t\u00e9rmica \u00e9 mais dif\u00edcil.\u00a0Est\u00e1 intimamente associado ao\u00a0<\/span><a title=\"O que \u00e9 entropia\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/what-is-entropy\/\"><strong><span>conceito de entropia<\/span><\/strong><\/a><span>\u00a0, que quantifica a energia de uma subst\u00e2ncia que n\u00e3o est\u00e1 mais dispon\u00edvel para realizar um trabalho \u00fatil.\u00a0Por exemplo, a eletricidade \u00e9 particularmente \u00fatil, pois possui\u00a0<strong>entropia\u00a0<\/strong><\/span><strong><span>muito\u00a0<\/span><\/strong><strong><span>baixa<\/span><\/strong><span>\u00a0(\u00e9 altamente ordenada) e pode ser convertida em outras formas de energia com\u00a0<\/span><strong><span>muita efici\u00eancia<\/span><\/strong><span>\u00a0.\u00a0Tenha cuidado ao compar\u00e1-lo com a efici\u00eancia da energia e\u00f3lica ou hidrel\u00e9trica (turbinas e\u00f3licas n\u00e3o s\u00e3o motores de calor), n\u00e3o h\u00e1 convers\u00e3o de energia entre a energia t\u00e9rmica e a mec\u00e2nica.<\/span><\/p>\n<p><span>A efici\u00eancia t\u00e9rmica de v\u00e1rios motores t\u00e9rmicos projetados ou usados \u200b\u200bhoje em dia tem uma grande variedade:<\/span><\/p>\n<p><strong><span>Por exemplo:<\/span><\/strong><\/p>\n<p><strong><span>Transporte<\/span><\/strong><\/p>\n<ul>\n<li><span>Em meados do s\u00e9culo XX, uma\u00a0<\/span><strong><span>locomotiva a vapor<\/span><\/strong><span>\u00a0t\u00edpica\u00a0tinha uma efici\u00eancia t\u00e9rmica de cerca de\u00a0<\/span><strong><span>6%<\/span><\/strong><span>\u00a0.\u00a0Isso significa que para cada 100 MJ de carv\u00e3o queimado, 6 MJ de pot\u00eancia mec\u00e2nica foram produzidos.<\/span><\/li>\n<li><span>Um\u00a0<\/span><strong><span>motor automotivo a gasolina<\/span><\/strong><span>\u00a0t\u00edpico\u00a0opera com cerca de\u00a0<\/span><strong><span>25% a 30%<\/span><\/strong><span>\u00a0de efici\u00eancia t\u00e9rmica.\u00a0Cerca de 70-75% \u00e9 rejeitado como calor residual sem ser convertido em trabalho \u00fatil, ou seja, trabalho entregue \u00e0s rodas.<\/span><\/li>\n<li><span>Um\u00a0<\/span><strong><span>motor automotivo a diesel<\/span><\/strong><span>\u00a0t\u00edpico\u00a0opera em torno de\u00a0<\/span><strong><span>30% a 35%<\/span><\/strong><span>\u00a0.\u00a0Em geral, os motores que usam o ciclo Diesel geralmente s\u00e3o mais eficientes.<\/span><\/li>\n<li><span>Em 2014, novos regulamentos foram introduzidos para\u00a0<\/span><strong><span>carros de F\u00f3rmula 1<\/span><\/strong><span>\u00a0.\u00a0Esses regulamentos sobre esportes a motor levaram as equipes a desenvolver unidades de pot\u00eancia altamente eficientes.\u00a0Segundo a Mercedes, sua unidade de pot\u00eancia est\u00e1 atingindo\u00a0<\/span><strong><span>mais de 45%<\/span><\/strong><span>\u00a0e quase 50% de efici\u00eancia t\u00e9rmica, ou seja, 45 a 50% da energia potencial do combust\u00edvel \u00e9 entregue \u00e0s rodas.<\/span><\/li>\n<li><span>O motor diesel tem a mais alta efici\u00eancia t\u00e9rmica de qualquer motor de combust\u00e3o pr\u00e1tico.\u00a0<\/span><strong><span>Os motores a diesel de baixa velocidade<\/span><\/strong><span>\u00a0(usados \u200b\u200bem navios) podem ter uma efici\u00eancia t\u00e9rmica superior a\u00a0<\/span><strong><span>50%<\/span><\/strong><span>\u00a0.\u00a0O maior motor diesel do mundo chega a 51,7%.<\/span><\/li>\n<\/ul>\n<p><strong><span>Engenharia de Energia<\/span><\/strong><\/p>\n<ul>\n<li><strong><span>Convers\u00e3o de energia t\u00e9rmica oce\u00e2nica (OTEC).\u00a0O OTEC<\/span><\/strong><span>\u00a0\u00e9 um motor t\u00e9rmico muito sofisticado que usa a diferen\u00e7a de temperatura entre \u00e1guas do mar mais frias e profundas da superf\u00edcie para acionar uma turbina de baixa press\u00e3o.\u00a0Como a\u00a0<\/span><strong><span>diferen\u00e7a de temperatura \u00e9 baixa<\/span><\/strong><span>\u00a0, cerca de 20 \u00b0 C, sua efici\u00eancia t\u00e9rmica tamb\u00e9m \u00e9 muito baixa,\u00a0<\/span><strong><span>cerca de 3%<\/span><\/strong><span>\u00a0.<\/span><\/li>\n<li><span>Nas modernas\u00a0<\/span><a title=\"Usina nuclear\" href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/\"><strong><span>usinas nucleares,<\/span><\/strong><\/a><span>\u00a0a efici\u00eancia t\u00e9rmica geral \u00e9 de cerca de\u00a0<\/span><strong><span>um ter\u00e7o<\/span><\/strong><span>\u00a0(33%); portanto, s\u00e3o necess\u00e1rios\u00a0<\/span><strong><span>3000 MWth<\/span><\/strong><span>\u00a0de energia t\u00e9rmica da rea\u00e7\u00e3o de fiss\u00e3o para gerar\u00a0<\/span><strong><span>1000 MWe<\/span><\/strong><span>\u00a0de energia el\u00e9trica.\u00a0Efici\u00eancias mais altas podem ser alcan\u00e7adas aumentando a\u00a0<\/span><strong><span>temperatura<\/span><\/strong><span>\u00a0do\u00a0<\/span><a title=\"Propriedades do Steam - O que \u00e9 o Steam\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-o-steam-propriedades-do-steam-definicao\/\"><span>vapor<\/span><\/a><span>\u00a0.\u00a0Mas isso requer um aumento nas press\u00f5es dentro de caldeiras ou\u00a0<\/span><a title=\"Gerador de vapor\" href=\"https:\/\/www.nuclear-power.com\/steam-generator\/\"><span>geradores de vapor<\/span><\/a><span>.\u00a0No entanto, considera\u00e7\u00f5es metal\u00fargicas imp\u00f5em limites superiores a essas press\u00f5es.\u00a0Em compara\u00e7\u00e3o com outras fontes de energia, a efici\u00eancia t\u00e9rmica de 33% n\u00e3o \u00e9 grande.\u00a0Mas deve-se notar que as usinas nucleares s\u00e3o muito mais complexas que as usinas de combust\u00edveis f\u00f3sseis e \u00e9 muito mais f\u00e1cil queimar combust\u00edveis f\u00f3sseis do que gerar energia a partir\u00a0<\/span><a title=\"Combust\u00edvel nuclear\" href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/nuclear-fuel\/\"><span>de combust\u00edveis nucleares<\/span><\/a><span>\u00a0.<\/span><\/li>\n<li><span>As usinas subcr\u00edticas de combust\u00edveis f\u00f3sseis, que s\u00e3o operadas sob\u00a0<\/span><strong><span>press\u00e3o cr\u00edtica<\/span><\/strong><span>\u00a0(ou seja, inferiores a 22,1 MPa), podem atingir uma efici\u00eancia de 36 a 40%.<\/span><\/li>\n<li><span>Os\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/reactor-types\/supercritical-water-reactor-scwr\/\"><strong><span>reatores supercr\u00edticos de \u00e1gua<\/span><\/strong><\/a><span>\u00a0s\u00e3o considerados um avan\u00e7o promissor para\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/\"><span>as usinas nucleares<\/span><\/a><span>\u00a0devido \u00e0 sua\u00a0<\/span><strong><span>alta efici\u00eancia t\u00e9rmica<\/span><\/strong><span>\u00a0(~ 45% vs. ~ 33% para as LWRs atuais).<\/span><\/li>\n<li><span>As usinas supercr\u00edticas de combust\u00edveis f\u00f3sseis, que s\u00e3o operadas sob\u00a0<\/span><strong><span>press\u00e3o supercr\u00edtica<\/span><\/strong><span>\u00a0(ou seja, superior a 22,1 MPa), t\u00eam efici\u00eancia em torno de\u00a0<\/span><strong><span>43%<\/span><\/strong><span>\u00a0.\u00a0As usinas el\u00e9tricas a carv\u00e3o mais eficientes e tamb\u00e9m muito complexas, operadas a\u00a0<strong>press\u00f5es\u00a0<\/strong><\/span><strong><span>&#8220;ultra-cr\u00edticas&#8221;<\/span><\/strong><span>\u00a0(ou seja, cerca de 30 MPa) e que utilizam reaquecimento em v\u00e1rios est\u00e1gios, atingem cerca de\u00a0<strong>48% de<\/strong>\u00a0efici\u00eancia.<\/span><\/li>\n<li><span>As modernas instala\u00e7\u00f5es de\u00a0<\/span><strong><span>turbina a g\u00e1s de ciclo combinado<\/span><\/strong><span>\u00a0(CCGT), nas quais o ciclo termodin\u00e2mico consiste em\u00a0<\/span><strong><span>dois ciclos de usina<\/span><\/strong><span>\u00a0(por exemplo, o ciclo de Brayton e o ciclo Rankine), podem atingir uma efici\u00eancia t\u00e9rmica de cerca de\u00a0<\/span><strong><span>55%<\/span><\/strong><span>\u00a0, em contraste com um vapor de ciclo \u00fanico usina, limitada a efici\u00eancias em torno de 35 a 45%.<\/span><\/li>\n<\/ul>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Efici\u00eancia t\u00e9rmica do ciclo de Brayton<\/span><\/h2>\n<p><span>Vamos assumir o\u00a0<\/span><strong><span>ciclo de Brayton ideal<\/span><\/strong><span>\u00a0que descreve o funcionamento de um\u00a0<strong>motor de calor com\u00a0<\/strong><\/span><strong><span>press\u00e3o constante<\/span><\/strong>\u00a0<span>.\u00a0<strong>Os modernos<\/strong>\u00a0motores de\u00a0<strong>turbina a g\u00e1s<\/strong>\u00a0e os motores a\u00a0<strong>jato de respira\u00e7\u00e3o<\/strong>\u00a0tamb\u00e9m seguem o ciclo de Brayton.\u00a0Esse ciclo consiste em quatro processos termodin\u00e2micos:<\/span><\/p>\n<ol>\n<li>\n<figure id=\"attachment_16843\" class=\"wp-caption alignright\" aria-describedby=\"caption-attachment-16843\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle.png\"><img loading=\"lazy\" class=\"size-medium wp-image-16843 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle-300x244.png\" alt=\"primeira lei - exemplo - ciclo de brayton\" width=\"300\" height=\"244\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle-300x244.png\" \/><\/a><figcaption id=\"caption-attachment-16843\" class=\"wp-caption-text\"><span>O ciclo ideal de Brayton consiste em quatro processos termodin\u00e2micos.\u00a0Dois processos isentr\u00f3picos e dois processos isob\u00e1ricos.<\/span><\/figcaption><\/figure>\n<p><strong><span>compress\u00e3o isentr\u00f3pica<\/span><\/strong><span>\u00a0&#8211; o ar ambiente \u00e9 aspirado para o compressor, onde \u00e9 pressurizado (1 \u2192 2).\u00a0O trabalho necess\u00e1rio para o compressor \u00e9 dado por\u00a0<\/span><strong><span>W\u00a0<\/span><\/strong><strong><sub><span>C<\/span><\/sub><\/strong><strong><span>\u00a0= H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><strong><span>\u00a0.<\/span><\/strong><\/li>\n<li><strong><span>adi\u00e7\u00e3o de calor isob\u00e1rico<\/span><\/strong><span>\u00a0&#8211; o ar comprimido passa por uma c\u00e2mara de combust\u00e3o, onde o combust\u00edvel \u00e9 queimado e o ar ou outro meio \u00e9 aquecido (2 \u2192 3).\u00a0\u00c9 um processo de press\u00e3o constante, j\u00e1 que a c\u00e2mara est\u00e1 aberta para entrar e sair.\u00a0O calor l\u00edquido adicionado \u00e9 dado por\u00a0<\/span><strong><span>Q\u00a0<\/span><\/strong><strong><sub><span>add<\/span><\/sub><\/strong><strong><span>\u00a0= H\u00a0<\/span><\/strong><strong><sub><span>3<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><\/li>\n<li><strong><span>expans\u00e3o isentr\u00f3pica<\/span><\/strong><span>\u00a0&#8211; o ar aquecido e pressurizado se expande na turbina, gasta sua energia.\u00a0O trabalho realizado pela turbina \u00e9 dado por\u00a0<\/span><strong><span>W\u00a0<\/span><\/strong><strong><sub><span>T<\/span><\/sub><\/strong><strong><span>\u00a0= H\u00a0<\/span><\/strong><strong><sub><span>4<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>3<\/span><\/sub><\/strong><\/li>\n<li><strong><span>rejei\u00e7\u00e3o de calor isob\u00e1rica<\/span><\/strong><span>\u00a0&#8211; o calor residual deve ser rejeitado para fechar o ciclo.\u00a0O calor l\u00edquido rejeitado \u00e9 dado por\u00a0<\/span><strong><span>Q\u00a0<\/span><\/strong><strong><sub><span>re<\/span><\/sub><\/strong><strong><span>\u00a0= H\u00a0<\/span><\/strong><strong><sub><span>4<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><\/li>\n<\/ol>\n<p><span>Como pode ser visto, podemos descrever e calcular (por exemplo, efici\u00eancia termodin\u00e2mica) esses ciclos (da mesma forma para o\u00a0<\/span><strong><span>ciclo de Rankine<\/span><\/strong><span>\u00a0) usando\u00a0<\/span><a title=\"O que \u00e9 entalpia\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/what-is-enthalpy\/\"><span>entalpias<\/span><\/a><span>\u00a0.<\/span><\/p>\n<p><span>Para calcular a\u00a0<\/span><strong><span>efici\u00eancia t\u00e9rmica<\/span><\/strong><span>\u00a0do\u00a0<\/span><strong><span>ciclo de Brayton<\/span><\/strong><span>\u00a0(compressor \u00fanico e turbina \u00fanica), os engenheiros usam a\u00a0<\/span><strong><span>primeira lei da termodin\u00e2mica<\/span><\/strong><span>\u00a0em termos de entalpia e n\u00e3o em energia interna.<\/span><\/p>\n<p><span>A\u00a0<\/span><a title=\"Primeira lei em termos de entalpia dH = dQ + Vdp\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/first-law-in-terms-of-enthalpy-dh-dq-vdp\/\"><span>primeira lei em termos de entalpia<\/span><\/a><span>\u00a0\u00e9:<\/span><\/p>\n<p><em><strong><span>dH = dQ + Vdp<\/span><\/strong><\/em><\/p>\n<p><span>Nesta equa\u00e7\u00e3o, o termo\u00a0<\/span><strong><em><span>Vdp<\/span><\/em><\/strong><span>\u00a0\u00e9 um\u00a0<\/span><strong><span>trabalho de processo de fluxo.\u00a0<\/span><\/strong><span>Este trabalho, \u00a0\u00a0<\/span><strong><em><span>Vdp<\/span><\/em><\/strong><span>\u00a0, \u00e9 usado para\u00a0<\/span><strong><span>sistemas de fluxo aberto,<\/span><\/strong><span>\u00a0como uma\u00a0<\/span><strong><span>turbina<\/span><\/strong><span>\u00a0ou uma\u00a0<\/span><strong><span>bomba<\/span><\/strong><span>\u00a0na qual existe um\u00a0<\/span><strong><span>&#8220;dp&#8221;<\/span><\/strong><span>\u00a0, ou seja, mudan\u00e7a de press\u00e3o.\u00a0N\u00e3o h\u00e1 altera\u00e7\u00f5es no\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/fluid-dynamics\/control-volume-control-volume-analysis\/\"><span>volume de controle<\/span><\/a><span>\u00a0.\u00a0Como pode ser visto, essa forma de lei\u00a0<\/span><strong><span>simplifica a descri\u00e7\u00e3o da transfer\u00eancia de energia<\/span><\/strong><span>\u00a0.<\/span><\/p>\n<p><span>Existem express\u00f5es em termos de vari\u00e1veis \u200b\u200bmais familiares, como\u00a0<\/span><a href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-temperatura-fisica-definicao\/\"><span>temperatura<\/span><\/a><span>\u00a0e\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-pressure-physics\/\"><span>press\u00e3o<\/span><\/a><span>\u00a0:<\/span><\/p>\n<p><strong><em><span>dH = C\u00a0<\/span><\/em><\/strong><strong><em><sub><span>p<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0dT + V (1-aT) dp<\/span><\/em><\/strong><\/p>\n<p><span>Onde\u00a0<\/span><strong><span>C\u00a0<\/span><\/strong><strong><sub><span>p<\/span><\/sub><\/strong><span>\u00a0\u00e9 a\u00a0<\/span><strong><a title=\"Capacidade t\u00e9rmica - Capacidade t\u00e9rmica espec\u00edfica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/heat-capacity\/\"><span>capacidade de calor<\/span><\/a><span>\u00a0a uma press\u00e3o constante<\/span><\/strong><span>\u00a0e\u00a0<\/span><strong><em><span>\u03b1<\/span><\/em><\/strong><span>\u00a0\u00e9 o coeficiente de expans\u00e3o t\u00e9rmica (c\u00fabico).\u00a0Para\u00a0<\/span><strong><span>o g\u00e1s ideal<\/span><\/strong><span>\u00a0\u03b1T = 1 e, portanto:<\/span><\/p>\n<p><strong><em><span>dH = C\u00a0<\/span><\/em><\/strong><strong><em><sub><span>p<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0dT<\/span><\/em><\/strong><\/p>\n<p><strong><span>A press\u00e3o constante<\/span><\/strong><span>\u00a0, a\u00a0<\/span><strong><span>mudan\u00e7a de entalpia<\/span><\/strong><span>\u00a0\u00e9 igual \u00e0\u00a0<\/span><strong><span>energia<\/span><\/strong><span>\u00a0transferida do ambiente atrav\u00e9s do aquecimento:<\/span><\/p>\n<p><strong><span>Processo isob\u00e1rico (Vdp = 0):<\/span><\/strong><\/p>\n<p><strong><span>dH = dQ \u2192 Q = H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><strong><span>\u00a0\u00a0\u00a0\u2192 H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><strong><span>\u00a0=\u00a0<\/span><em><span>C\u00a0<\/span><\/em><\/strong><strong><em><sub><span>P<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0(T\u00a0<\/span><\/em><\/strong><strong><em><sub><span>2<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0&#8211; T\u00a0<\/span><\/em><\/strong><strong><em><sub><span>1<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0)<\/span><\/em><\/strong><\/p>\n<p><strong><span>Na entropia constante<\/span><\/strong><span>\u00a0, ou seja, no processo isentr\u00f3pico, a\u00a0<\/span><strong><span>mudan\u00e7a de entalpia<\/span><\/strong><span>\u00a0\u00e9 igual ao\u00a0<\/span><strong><span>trabalho do processo de fluxo<\/span><\/strong><span>\u00a0realizado no ou pelo sistema:<\/span><\/p>\n<p><strong><span>Processo isentr\u00f3pico (dQ = 0):<\/span><\/strong><\/p>\n<p><strong><span>dH = Vdp \u2192 W = H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><strong><span>\u00a0\u00a0\u00a0\u00a0\u00a0\u2192 H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><strong><span>\u00a0=\u00a0<\/span><em><span>C\u00a0<\/span><\/em><\/strong><strong><em><sub><span>P<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0(T\u00a0<\/span><\/em><\/strong><strong><em><sub><span>2<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0&#8211; T\u00a0<\/span><\/em><\/strong><strong><em><sub><span>1<\/span><\/sub><\/em><\/strong><strong><em><span>\u00a0)<\/span><\/em><\/strong><\/p>\n<figure id=\"attachment_16843\" class=\"wp-caption alignright\" aria-describedby=\"caption-attachment-16843\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle.png\"><img loading=\"lazy\" class=\"size-medium wp-image-16843 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle-300x244.png\" alt=\"primeira lei - exemplo - ciclo de brayton\" width=\"300\" height=\"244\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/first-law-example-brayton-cycle-300x244.png\" \/><\/a><figcaption id=\"caption-attachment-16843\" class=\"wp-caption-text\"><span>O ciclo ideal de Brayton consiste em quatro processos termodin\u00e2micos.\u00a0Dois processos isentr\u00f3picos e dois processos isob\u00e1ricos.<\/span><\/figcaption><\/figure>\n<p><span>A\u00a0<\/span><strong><span>entalpia<\/span><\/strong><span>\u00a0pode ser transformada em uma\u00a0vari\u00e1vel\u00a0<\/span><strong><span>intensiva<\/span><\/strong><span>\u00a0ou\u00a0<\/span><strong><span>espec\u00edfica<\/span><\/strong><span>\u00a0dividindo-se pela\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-mass-and-weight\/what-is-mass\/\"><span>massa<\/span><\/a><span>\u00a0.\u00a0<\/span><strong><span>Os engenheiros usam mais a\u00a0<\/span><\/strong><strong><span>entalpia espec\u00edfica<\/span><\/strong><span>\u00a0na an\u00e1lise termodin\u00e2mica do que a pr\u00f3pria entalpia.\u00a0A efici\u00eancia t\u00e9rmica desse ciclo simples de Brayton, para o g\u00e1s ideal e em termos de entalpias espec\u00edficas, agora pode ser expressa em termos de temperatura:<\/span><\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-brayton-cycle-equation.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-16963 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-brayton-cycle-equation.png\" alt=\"efici\u00eancia t\u00e9rmica do ciclo de Brayton\" width=\"602\" height=\"60\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-brayton-cycle-equation.png\" \/><\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Efici\u00eancia t\u00e9rmica do ciclo Rankine<\/span><\/h2>\n<figure id=\"attachment_16026\" class=\"wp-caption alignright\" aria-describedby=\"caption-attachment-16026\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Thermodynamic-Cycles-min.png\"><img loading=\"lazy\" class=\"size-medium wp-image-16026 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Thermodynamic-Cycles-min-300x277.png\" alt=\"termodin\u00e2mica de engenharia\" width=\"300\" height=\"277\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Thermodynamic-Cycles-min-300x277.png\" \/><\/a><figcaption id=\"caption-attachment-16026\" class=\"wp-caption-text\"><span>Ciclo de Rankine &#8211; Termodin\u00e2mica como ci\u00eancia de convers\u00e3o de energia<\/span><\/figcaption><\/figure>\n<p><span>O\u00a0<\/span><strong><span>ciclo Rankine<\/span><\/strong><span>\u00a0descreve de perto os processos em motores t\u00e9rmicos a vapor comumente encontrados na maioria das\u00a0<\/span><strong><span>usinas termel\u00e9tricas<\/span><\/strong><span>\u00a0.\u00a0As fontes de calor usadas nessas usinas s\u00e3o geralmente a combust\u00e3o de combust\u00edveis f\u00f3sseis, como carv\u00e3o, g\u00e1s natural ou tamb\u00e9m a\u00a0<\/span><strong><span>fiss\u00e3o nuclear<\/span><\/strong><span>\u00a0.<\/span><\/p>\n<p><span>Uma\u00a0<\/span><a title=\"Usina nuclear\" href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/\"><strong><span>usina<\/span><\/strong><\/a><span>\u00a0nuclear (\u00a0<a title=\"Usina nuclear\" href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/\"><strong>usina<\/strong><\/a>\u00a0nuclear) parece uma usina termel\u00e9trica padr\u00e3o, com uma exce\u00e7\u00e3o.\u00a0A fonte de calor na usina nuclear \u00e9 um\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/nuclear-reactor\/\"><strong><span>reator nuclear<\/span><\/strong><\/a><span>\u00a0.\u00a0Como \u00e9 t\u00edpico em todas as centrais t\u00e9rmicas convencionais, o calor \u00e9 usado para gerar\u00a0<\/span><a title=\"Propriedades do Steam - O que \u00e9 o Steam\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-o-steam-propriedades-do-steam-definicao\/\"><span>vapor<\/span><\/a><span>\u00a0que aciona uma turbina a vapor conectada a um gerador que produz eletricidade.<\/span><\/p>\n<p><span>Normalmente, a maioria das\u00a0<\/span><strong><span>usinas nucleares<\/span><\/strong><span>\u00a0opera\u00a0<\/span><strong><span>turbinas a vapor de condensa\u00e7\u00e3o de v\u00e1rios est\u00e1gios<\/span><\/strong><span>\u00a0.\u00a0Nessas turbinas, o est\u00e1gio de alta press\u00e3o recebe\u00a0<\/span><a href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-o-steam-propriedades-do-steam-definicao\/\"><span>vapor<\/span><\/a><span>\u00a0(esse vapor \u00e9 quase saturado &#8211; x = 0,995 &#8211; ponto C na figura;\u00a0<\/span><strong><span>6 MPa<\/span><\/strong><span>\u00a0; 275,6 \u00b0 C) de um gerador de vapor e o esgota para o separador-reaquecedor de umidade (ponto D )\u00a0O vapor deve ser reaquecido para evitar danos que possam ser causados \u200b\u200b\u00e0s p\u00e1s da turbina a vapor por vapor de\u00a0<\/span><a title=\"Qualidade de Vapor - Fra\u00e7\u00e3o de Secura\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/materials-nuclear-engineering\/properties-steam-what-is-steam\/vapor-quality-dryness-fraction\/\"><span>baixa qualidade<\/span><\/a><span>\u00a0.\u00a0O reaquecedor aquece o vapor (ponto D) e, em seguida, o vapor \u00e9 direcionado para o est\u00e1gio de baixa press\u00e3o da turbina a vapor, onde se expande (pontos E a F).\u00a0O vapor exaurido condensa no condensador e est\u00e1 a uma press\u00e3o bem abaixo da atmosf\u00e9rica (press\u00e3o absoluta de<\/span><strong><span>0,008 MPa<\/span><\/strong><span>\u00a0) e est\u00e1 em um estado parcialmente condensado (ponto F), tipicamente com uma qualidade pr\u00f3xima a 90%.<\/span><\/p>\n<p><span>Nesse caso, geradores de vapor, turbinas a vapor, condensadores e bombas de \u00e1gua de alimenta\u00e7\u00e3o constituem um motor t\u00e9rmico, sujeito \u00e0s limita\u00e7\u00f5es de efici\u00eancia impostas pela\u00a0<a title=\"Segunda Lei da Termodin\u00e2mica\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-a-segunda-lei-da-termodinamica-definicao\/\"><strong>segunda lei da termodin\u00e2mica<\/strong><\/a>\u00a0.\u00a0No caso ideal (sem atrito, processos revers\u00edveis, design perfeito), este motor t\u00e9rmico teria uma\u00a0<a title=\"Efici\u00eancia de Carnot - Efici\u00eancia do mecanismo de calor de Carnot\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/carnot-efficiency-efficiency-of-carnot-heat-engine\/\">efici\u00eancia<\/a>\u00a0de\u00a0<a title=\"Efici\u00eancia de Carnot - Efici\u00eancia do mecanismo de calor de Carnot\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/second-law-of-thermodynamics\/carnot-efficiency-efficiency-of-carnot-heat-engine\/\">Carnot<\/a>\u00a0de<\/span><\/p>\n<p><span>= 1 &#8211; T\u00a0<\/span><sub><span>frio<\/span><\/sub><span>\u00a0\/ T\u00a0<\/span><sub><span>quente<\/span><\/sub><span>\u00a0= 1 &#8211; 315\/549 = 42,6%<\/span><\/p>\n<p><span>onde a temperatura do reservat\u00f3rio quente \u00e9 de 275,6 \u00b0 C (548,7 K), a temperatura do reservat\u00f3rio frio \u00e9 de 41,5 \u00b0 C (314,7 K).\u00a0Mas a usina nuclear \u00e9 o\u00a0<\/span><strong><span>verdadeiro motor t\u00e9rmico<\/span><\/strong><span>\u00a0, no qual os processos termodin\u00e2micos s\u00e3o de alguma forma irrevers\u00edveis.\u00a0Eles n\u00e3o s\u00e3o feitos infinitamente devagar.\u00a0Em dispositivos reais (como turbinas, bombas e compressores), um atrito mec\u00e2nico e perdas de calor causam mais perdas de efici\u00eancia.<\/span><\/p>\n<p><span>Para calcular a\u00a0<\/span><strong><span>efici\u00eancia t\u00e9rmica<\/span><\/strong><span>\u00a0do\u00a0<\/span><strong><span>ciclo Rankine<\/span><\/strong><span>\u00a0mais simples\u00a0(sem reaquecer), os engenheiros usam a\u00a0<\/span><a title=\"Primeira lei em termos de entalpia dH = dQ + Vdp\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/first-law-in-terms-of-enthalpy-dh-dq-vdp\/\"><strong><span>primeira lei da termodin\u00e2mica em termos de entalpia<\/span><\/strong><\/a><span>\u00a0e n\u00e3o em energia interna.<\/span><\/p>\n<p><span>A primeira lei em termos de entalpia \u00e9:<\/span><\/p>\n<p><em><strong><span>dH = dQ + Vdp<\/span><\/strong><\/em><\/p>\n<p><span>Nesta equa\u00e7\u00e3o, o termo\u00a0<\/span><strong><em><span>Vdp<\/span><\/em><\/strong><span>\u00a0\u00e9 um\u00a0<\/span><strong><span>trabalho de processo de fluxo.\u00a0<\/span><\/strong><span>Este trabalho, \u00a0\u00a0<\/span><strong><em><span>Vdp<\/span><\/em><\/strong><span>\u00a0, \u00e9 usado para\u00a0<\/span><strong><span>sistemas de fluxo aberto,<\/span><\/strong><span>\u00a0como uma\u00a0<\/span><strong><span>turbina<\/span><\/strong><span>\u00a0ou uma\u00a0<\/span><strong><span>bomba<\/span><\/strong><span>\u00a0na qual existe um\u00a0<\/span><strong><span>&#8220;dp&#8221;<\/span><\/strong><span>\u00a0, ou seja, mudan\u00e7a de press\u00e3o.\u00a0N\u00e3o h\u00e1 altera\u00e7\u00f5es no\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/fluid-dynamics\/control-volume-control-volume-analysis\/\"><span>volume de controle<\/span><\/a><span>\u00a0.\u00a0Como pode ser visto, essa forma de lei\u00a0<\/span><strong><span>simplifica a descri\u00e7\u00e3o da transfer\u00eancia de energia<\/span><\/strong><span>\u00a0.\u00a0<\/span><strong><span>A press\u00e3o constante<\/span><\/strong><span>\u00a0, a\u00a0<\/span><strong><span>mudan\u00e7a de entalpia<\/span><\/strong><span>\u00a0\u00e9 igual \u00e0\u00a0<\/span><strong><span>energia<\/span><\/strong><span>\u00a0transferida do ambiente atrav\u00e9s do aquecimento:<\/span><\/p>\n<p><strong><span>Processo isob\u00e1rico (Vdp = 0):<\/span><\/strong><\/p>\n<p><strong><span>dH = dQ \u2192 Q = H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><\/p>\n<p><strong><span>Na entropia constante<\/span><\/strong><span>\u00a0, ou seja, no processo isentr\u00f3pico, a\u00a0<\/span><strong><span>mudan\u00e7a de entalpia<\/span><\/strong><span>\u00a0\u00e9 igual ao\u00a0<\/span><strong><span>trabalho do processo de fluxo<\/span><\/strong><span>\u00a0realizado no ou pelo sistema:<\/span><\/p>\n<p><strong><span>Processo isentr\u00f3pico (dQ = 0):<\/span><\/strong><\/p>\n<p><strong><span>dH = Vdp \u2192 W = H\u00a0<\/span><\/strong><strong><sub><span>2<\/span><\/sub><\/strong><strong><span>\u00a0&#8211; H\u00a0<\/span><\/strong><strong><sub><span>1<\/span><\/sub><\/strong><\/p>\n<p><span>\u00c9 \u00f3bvio que ser\u00e1 muito \u00fatil na an\u00e1lise de ambos os ciclos termodin\u00e2micos usados \u200b\u200bna engenharia de energia, ou seja, no ciclo de Brayton e no ciclo de Rankine.<\/span><\/p>\n<p><span>A\u00a0<\/span><strong><span>entalpia<\/span><\/strong><span>\u00a0pode ser transformada em uma\u00a0vari\u00e1vel\u00a0<\/span><strong><span>intensiva<\/span><\/strong><span>\u00a0ou\u00a0<\/span><strong><span>espec\u00edfica<\/span><\/strong><span>\u00a0dividindo-se pela\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-mass-and-weight\/what-is-mass\/\"><span>massa<\/span><\/a><span>\u00a0.\u00a0<\/span><strong><span>Os engenheiros usam mais a\u00a0<\/span><\/strong><strong><span>entalpia espec\u00edfica<\/span><\/strong><span>\u00a0na an\u00e1lise termodin\u00e2mica do que a pr\u00f3pria entalpia.\u00a0Ele \u00e9 tabulado nas\u00a0<\/span><a title=\"Tabelas de Vapor - Propriedades Espec\u00edficas da \u00c1gua e Vapor\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/steam-tables\/\"><strong><span>tabelas de vapor,<\/span><\/strong><\/a><span>\u00a0juntamente com o\u00a0<\/span><a title=\"O que \u00e9 volume espec\u00edfico\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-specific-volume\/\"><span>volume\u00a0<\/span><\/a><a title=\"Energia interna espec\u00edfica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/internal-energy-thermal-energy\/specific-internal-energy\/\"><span>espec\u00edfico<\/span><\/a><span>\u00a0e\u00a0<a title=\"Energia interna espec\u00edfica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/internal-energy-thermal-energy\/specific-internal-energy\/\">a energia interna espec\u00edfica<\/a>\u00a0.\u00a0A efici\u00eancia t\u00e9rmica desse ciclo simples de Rankine e em termos de entalpias espec\u00edficas seria:<\/span><\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-rankine-cycle-equation.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-16962 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-rankine-cycle-equation.png\" alt=\"efici\u00eancia t\u00e9rmica do ciclo Rankine\" width=\"535\" height=\"68\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-rankine-cycle-equation.png\" \/><\/a><\/p>\n<p><span>\u00c9 uma equa\u00e7\u00e3o muito simples e, para determinar a efici\u00eancia t\u00e9rmica, voc\u00ea pode usar os dados das\u00a0<\/span><strong><span>tabelas de vapor<\/span><\/strong><span>\u00a0.<\/span><\/p>\n<p><span>Nas modernas usinas nucleares, a efici\u00eancia t\u00e9rmica geral \u00e9 de cerca de\u00a0<\/span><strong><span>um ter\u00e7o<\/span><\/strong><span>\u00a0(33%); portanto, s\u00e3o necess\u00e1rios\u00a0<\/span><strong><span>3000 MWth<\/span><\/strong><span>\u00a0de energia t\u00e9rmica da rea\u00e7\u00e3o de fiss\u00e3o para gerar\u00a0<\/span><strong><span>1000 MWe<\/span><\/strong><span>\u00a0de energia el\u00e9trica.\u00a0O motivo est\u00e1 na temperatura do vapor relativamente baixa (\u00a0<\/span><strong><span>6 MPa<\/span><\/strong><span>\u00a0; 275,6 \u00b0 C).\u00a0Efici\u00eancias mais altas podem ser alcan\u00e7adas aumentando a\u00a0<\/span><strong><span>temperatura<\/span><\/strong><span>do vapor.\u00a0Mas isso requer um aumento nas press\u00f5es dentro de caldeiras ou geradores de vapor.\u00a0No entanto, considera\u00e7\u00f5es metal\u00fargicas imp\u00f5em limites superiores a essas press\u00f5es.\u00a0Em compara\u00e7\u00e3o com outras fontes de energia, a efici\u00eancia t\u00e9rmica de 33% n\u00e3o \u00e9 grande.\u00a0Mas deve-se notar que as usinas nucleares s\u00e3o muito mais complexas que as usinas de combust\u00edveis f\u00f3sseis e \u00e9 muito mais f\u00e1cil queimar combust\u00edveis f\u00f3sseis do que gerar energia a partir de combust\u00edveis nucleares.\u00a0As usinas subcr\u00edticas de combust\u00edveis f\u00f3sseis, que s\u00e3o operadas sob\u00a0<\/span><strong><span>press\u00e3o cr\u00edtica<\/span><\/strong><span>\u00a0(ou seja, inferiores a 22,1 MPa), podem atingir uma efici\u00eancia de 36 a 40%.<\/span><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;.<\/p>\n<p>Este artigo \u00e9 baseado na tradu\u00e7\u00e3o autom\u00e1tica do artigo original em ingl\u00eas. Para mais informa\u00e7\u00f5es, consulte o artigo em ingl\u00eas. Voc\u00ea pode nos ajudar. Se voc\u00ea deseja corrigir a tradu\u00e7\u00e3o, envie-a para: translations@nuclear-power.com ou preencha o formul\u00e1rio de tradu\u00e7\u00e3o on-line. Agradecemos sua ajuda, atualizaremos a tradu\u00e7\u00e3o o mais r\u00e1pido poss\u00edvel. Obrigado.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>A efici\u00eancia t\u00e9rmica, \u03b7\u00aa, de qualquer motor t\u00e9rmico \u00e9 definida como a raz\u00e3o entre o trabalho e a entrada de calor.\u00a0Para calcular a efici\u00eancia t\u00e9rmica, os engenheiros costumam usar entalpia.\u00a0Engenharia T\u00e9rmica Efici\u00eancia t\u00e9rmica Um\u00a0mecanismo t\u00e9rmico ideal\u00a0\u00e9 um mecanismo imagin\u00e1rio no qual a energia extra\u00edda como calor do reservat\u00f3rio de alta temperatura \u00e9 convertida completamente em &#8230; <a title=\"O que \u00e9 efici\u00eancia t\u00e9rmica &#8211; Defini\u00e7\u00e3o\" class=\"read-more\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-eficiencia-termica-definicao\/\" aria-label=\"More on O que \u00e9 efici\u00eancia t\u00e9rmica &#8211; Defini\u00e7\u00e3o\">Ler mais<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[14],"tags":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v15.4 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>O que \u00e9 efici\u00eancia t\u00e9rmica - Defini\u00e7\u00e3o<\/title>\n<meta name=\"description\" content=\"A efici\u00eancia t\u00e9rmica, \u03b7\u00aa, de qualquer motor t\u00e9rmico \u00e9 definida como a raz\u00e3o entre o trabalho e a entrada de calor. 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