{"id":48115,"date":"2019-11-08T05:12:13","date_gmt":"2019-11-08T04:12:13","guid":{"rendered":"https:\/\/www.thermal-engineering.org\/o-que-e-a-lei-dos-gases-definicao\/"},"modified":"2020-01-27T14:13:37","modified_gmt":"2020-01-27T13:13:37","slug":"o-que-e-a-lei-dos-gases-definicao","status":"publish","type":"post","link":"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-a-lei-dos-gases-definicao\/","title":{"rendered":"O que \u00e9 a lei dos gases &#8211; Defini\u00e7\u00e3o"},"content":{"rendered":"<div class=\"su-quote su-quote-style-default\">\n<div class=\"su-quote-inner su-clearfix\">Em geral, as leis dos gases s\u00e3o as primeiras equa\u00e7\u00f5es de estado, que correlacionam densidades de gases e l\u00edquidos a temperaturas e press\u00f5es.\u00a0As leis de g\u00e1s foram completamente desenvolvidas no final do s\u00e9culo XVIII.\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>Leis do g\u00e1s<\/h2>\n<p>Em geral, as\u00a0<strong>leis<\/strong>\u00a0dos\u00a0<strong>gases<\/strong>\u00a0s\u00e3o as\u00a0<strong>primeiras\u00a0<a title=\"Equa\u00e7\u00e3o de estado\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-equacao-de-estado-definicao\/\">equa\u00e7\u00f5es de estado<\/a><\/strong>\u00a0, que correlacionam densidades de gases e l\u00edquidos a temperaturas e press\u00f5es.\u00a0As\u00a0<strong>leis de g\u00e1s<\/strong>\u00a0foram completamente desenvolvidas no final do s\u00e9culo XVIII.\u00a0Essas leis ou declara\u00e7\u00f5es\u00a0<strong>precederam<\/strong>\u00a0a\u00a0<strong>lei dos gases ideais<\/strong>\u00a0, uma vez que, individualmente, essas leis s\u00e3o consideradas casos especiais da equa\u00e7\u00e3o do g\u00e1s ideal, com uma ou mais vari\u00e1veis \u200b\u200bmantidas constantes.\u00a0Como eles foram quase completamente substitu\u00eddos pela equa\u00e7\u00e3o de g\u00e1s ideal, n\u00e3o \u00e9 comum que os alunos aprendam essas leis em detalhes.\u00a0A\u00a0<strong>equa\u00e7\u00e3o do g\u00e1s ideal<\/strong> foi declarada pela primeira vez por \u00c9mile Clapeyron em 1834 como uma combina\u00e7\u00e3o dessas leis:<\/p>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-60 lgc-tablet-grid-60 lgc-mobile-grid-100 lgc-equal-heights  lgc-first\">\n<div class=\"inside-grid-column\">\n<h2><span>Lei de Boyle-Mariotte<\/span><\/h2>\n<p><strong><span>A lei de Boyle-Mariotte<\/span><\/strong><span>\u00a0\u00e9 uma das leis de g\u00e1s.\u00a0No final do s\u00e9culo XVII, Robert William Boyle e Edme Mariotte estudaram independentemente a rela\u00e7\u00e3o entre o\u00a0<\/span><strong><span>volume<\/span><\/strong><span>\u00a0e a\u00a0<\/span><strong><span>press\u00e3o<\/span><\/strong><span>\u00a0de um g\u00e1s\u00a0<\/span><strong><span>a temperatura constante<\/span><\/strong><span>\u00a0.\u00a0Os resultados de certas experi\u00eancias com gases sob press\u00e3o relativamente baixa levaram Robert Boyle a formular uma lei bem conhecida.\u00a0Afirma que:<\/span><\/p>\n<p><em><span>Para uma massa fixa de g\u00e1s a temperatura constante, o volume \u00e9 inversamente proporcional \u00e0 press\u00e3o.<\/span><\/em><\/p>\n<p><span>Isso significa que, por exemplo, se voc\u00ea aumentar o volume 10 vezes, a press\u00e3o diminuir\u00e1 10 vezes.\u00a0Se voc\u00ea reduzir pela metade o volume, dobrar\u00e1 a press\u00e3o.<\/span><\/p>\n<p><span>Voc\u00ea pode expressar isso matematicamente como:<\/span><\/p>\n<p><strong><em><span>pV = constante<\/span><\/em><\/strong><\/p>\n<p><i><span>ou<\/span><\/i><\/p>\n<p><strong><em><span>p\u00a0<\/span><sub><span>1<\/span><\/sub><span>\u00a0V\u00a0<\/span><sub><span>1<\/span><\/sub><span>\u00a0= p\u00a0<\/span><sub><span>2<\/span><\/sub><span>\u00a0V\u00a0<\/span><sub><span>2<\/span><\/sub><\/em><\/strong><\/p>\n<p><span>Sim, parece ser id\u00eantico ao\u00a0<\/span><strong><span>processo isot\u00e9rmico<\/span><\/strong><span>\u00a0do g\u00e1s ideal.\u00a0De fato, durante seus experimentos, a temperatura permanece constante, como foi assumido por Mariotte.\u00a0Esses resultados s\u00e3o totalmente consistentes com\u00a0<\/span><strong><span>a lei ideal dos gases<\/span><\/strong><span>\u00a0, que determina que a constante \u00e9 igual a\u00a0<\/span><strong><span>nRT<\/span><\/strong><span>\u00a0.<\/span><\/p>\n<p><strong><em><span>pV = nRT<\/span><\/em><\/strong><\/p>\n<p><span>Onde:<\/span><\/p>\n<ul>\n<li><em><span>p<\/span><\/em><span>\u00a0\u00e9 a press\u00e3o absoluta do g\u00e1s<\/span><\/li>\n<li><em><span>n<\/span><\/em><span>\u00a0\u00e9 a quantidade de subst\u00e2ncia<\/span><\/li>\n<li><em><span>T<\/span><\/em><span>\u00a0\u00e9 a temperatura absoluta<\/span><\/li>\n<li><em><span>V<\/span><\/em><span>\u00a0\u00e9 o volume<\/span><\/li>\n<li><em><span>R<\/span><\/em><span>\u00a0\u00a0\u00e9 a constante de g\u00e1s ideal, ou universal, igual ao produto da constante de Boltzmann e da constante de Avogadro,<\/span><\/li>\n<\/ul>\n<p><span>Nesta equa\u00e7\u00e3o, o s\u00edmbolo R \u00e9 uma constante chamada constante universal de g\u00e1s que tem o mesmo valor para todos os gases &#8211; ou seja, R = 8,31 J \/ mol K.<\/span><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-40 lgc-tablet-grid-40 lgc-mobile-grid-100 lgc-equal-heights  lgc-last\">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17319\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17319\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boyle-Mariotte-Law.gif\"><img loading=\"lazy\" class=\"wp-image-17319 size-full lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boyle-Mariotte-Law.gif\" alt=\"Lei de Boyle-Mariotte\" width=\"532\" height=\"403\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boyle-Mariotte-Law.gif\" \/><\/a><figcaption id=\"caption-attachment-17319\" class=\"wp-caption-text\"><span>Para uma massa fixa de g\u00e1s a temperatura constante, o volume \u00e9 inversamente proporcional \u00e0 press\u00e3o.\u00a0Fonte: grc.nasa.gov A pol\u00edtica de direitos autorais da NASA afirma que \u201co material da NASA n\u00e3o \u00e9 protegido por direitos autorais, a menos que seja observado\u201d.<\/span><\/figcaption><\/figure>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-60 lgc-tablet-grid-60 lgc-mobile-grid-100 lgc-equal-heights  lgc-first\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Lei de Charles<\/span><\/h2>\n<p><strong><span>A lei de Charles<\/span><\/strong><span>\u00a0\u00e9 uma das leis de g\u00e1s.\u00a0No final do s\u00e9culo XVIII, o inventor e cientista franc\u00eas\u00a0<\/span><strong><span>Jacques Alexandre C\u00e9sar Charles<\/span><\/strong><span>\u00a0estudou a rela\u00e7\u00e3o entre o\u00a0<\/span><strong><span>volume<\/span><\/strong><span>\u00a0e a\u00a0<\/span><strong><span>temperatura<\/span><\/strong><span>\u00a0de um g\u00e1s\u00a0<\/span><strong><span>sob press\u00e3o constante<\/span><\/strong><span>\u00a0.\u00a0Os resultados de certas experi\u00eancias com gases sob press\u00e3o relativamente baixa levaram Jacques Alexandre C\u00e9sar Charles a formular uma lei bem conhecida.\u00a0Afirma que:<\/span><\/p>\n<p><em><span>Para uma massa fixa de g\u00e1s a press\u00e3o constante, o volume \u00e9 diretamente proporcional \u00e0 temperatura Kelvin.<\/span><\/em><\/p>\n<p><span>Isso significa que, por exemplo, se voc\u00ea dobrar a temperatura, dobrar\u00e1 o volume.\u00a0Se voc\u00ea reduzir pela metade a temperatura, reduzir\u00e1 pela metade o volume.<\/span><\/p>\n<p><span>Voc\u00ea pode expressar isso matematicamente como:<\/span><\/p>\n<p><strong><em><span>V = constante.\u00a0T<\/span><\/em><\/strong><\/p>\n<p><span>Sim, parece ser id\u00eantico ao\u00a0<\/span><strong><span>processo isob\u00e1rico<\/span><\/strong><span>\u00a0do g\u00e1s ideal.\u00a0Esses resultados s\u00e3o totalmente consistentes com\u00a0<\/span><strong><span>a lei ideal dos gases<\/span><\/strong><span>\u00a0, que determina que a constante \u00e9 igual a\u00a0<\/span><strong><span>nR \/ p<\/span><\/strong><span>\u00a0.\u00a0Se voc\u00ea reorganizar a equa\u00e7\u00e3o pV = nRT dividindo os dois lados por p, obter\u00e1:<\/span><\/p>\n<p><strong><em><span>V = nR \/ p.\u00a0T<\/span><\/em><\/strong><\/p>\n<p><span>onde nR \/ p \u00e9 constante e:<\/span><\/p>\n<ul>\n<li><em><span>p<\/span><\/em><span>\u00a0\u00e9 a press\u00e3o absoluta do g\u00e1s<\/span><\/li>\n<li><em><span>n<\/span><\/em><span>\u00a0\u00e9 a quantidade de subst\u00e2ncia<\/span><\/li>\n<li><em><span>T<\/span><\/em><span>\u00a0\u00e9 a temperatura absoluta<\/span><\/li>\n<li><em><span>V<\/span><\/em><span>\u00a0\u00e9 o volume<\/span><\/li>\n<li><em><span>R<\/span><\/em><span>\u00a0\u00a0\u00e9 a constante de g\u00e1s ideal, ou universal, igual ao produto da constante de Boltzmann e da constante de Avogadro,<\/span><\/li>\n<\/ul>\n<p><span>Nesta equa\u00e7\u00e3o, o s\u00edmbolo R \u00e9 uma constante chamada constante universal de g\u00e1s que tem o mesmo valor para todos os gases &#8211; ou seja, R = 8,31 J \/ mol K.<\/span><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-40 lgc-tablet-grid-40 lgc-mobile-grid-100 lgc-equal-heights  lgc-last\">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17320\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17320\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Charles-Law.gif\"><img loading=\"lazy\" class=\"wp-image-17320 size-full lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Charles-Law.gif\" alt=\"A lei de Charles \u00e9 uma das leis de g\u00e1s.\" width=\"533\" height=\"403\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Charles-Law.gif\" \/><\/a><figcaption id=\"caption-attachment-17320\" class=\"wp-caption-text\"><span>Para uma massa fixa de g\u00e1s a press\u00e3o constante, o volume \u00e9 diretamente proporcional \u00e0 temperatura Kelvin.\u00a0Fonte: grc.nasa.gov A pol\u00edtica de direitos autorais da NASA afirma que \u201co material da NASA n\u00e3o \u00e9 protegido por direitos autorais, a menos que seja observado\u201d.<\/span><\/figcaption><\/figure>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-60 lgc-tablet-grid-60 lgc-mobile-grid-100 lgc-equal-heights  lgc-first\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Lei de Guy-Lussac<\/span><\/h2>\n<p><strong><span>A lei de Guy-Lussac<\/span><\/strong><span>\u00a0ou a\u00a0<\/span><strong><span>lei de press\u00e3o<\/span><\/strong><span>\u00a0\u00e9 uma das leis de g\u00e1s.\u00a0No final do s\u00e9culo 18 e in\u00edcio do s\u00e9culo 19, foi descoberto pelo qu\u00edmico franc\u00eas\u00a0<\/span><strong><span>Joseph Louis Gay-Lussac<\/span><\/strong><span>\u00a0.\u00a0Ele estudou a rela\u00e7\u00e3o entre a\u00a0<\/span><strong><span>press\u00e3o<\/span><\/strong><span>\u00a0e a\u00a0<\/span><strong><span>temperatura<\/span><\/strong><span>\u00a0de um g\u00e1s em\u00a0<\/span><strong><span>volume constante<\/span><\/strong><span>\u00a0.\u00a0Os resultados de certas experi\u00eancias com gases sob press\u00e3o relativamente baixa levaram Joseph Louis Gay-Lussac a formular uma conhecida &#8221;\u00a0<\/span><strong><span>lei da press\u00e3o<\/span><\/strong><span>\u00a0&#8220;.\u00a0Afirma que:<\/span><\/p>\n<p><em><span>Para uma massa fixa de g\u00e1s em volume constante, a press\u00e3o \u00e9 diretamente proporcional \u00e0 temperatura Kelvin.<\/span><\/em><\/p>\n<p><span>Isso significa que, por exemplo, se voc\u00ea dobrar a temperatura, dobrar\u00e1 a press\u00e3o.\u00a0Se voc\u00ea reduzir pela metade a temperatura, reduzir\u00e1 a press\u00e3o pela metade.<\/span><\/p>\n<p><span>Voc\u00ea pode expressar isso matematicamente como:<\/span><\/p>\n<p><strong><em><span>p = constante.\u00a0T<\/span><\/em><\/strong><\/p>\n<p><span>Sim, parece ser id\u00eantico ao processo isoc\u00f3rico do g\u00e1s ideal.\u00a0Esses resultados s\u00e3o totalmente consistentes com a lei ideal dos gases, que determina que a constante \u00e9 igual a nR \/ V.\u00a0Se voc\u00ea reorganizar a equa\u00e7\u00e3o pV = nRT dividindo os dois lados por V, obter\u00e1:<\/span><\/p>\n<p><strong><em><span>p = nR \/ V.\u00a0T<\/span><\/em><\/strong><\/p>\n<p><span>onde nR \/ V \u00e9 constante e:<\/span><\/p>\n<ul>\n<li><em><span>p<\/span><\/em><span>\u00a0\u00e9 a press\u00e3o absoluta do g\u00e1s<\/span><\/li>\n<li><em><span>n<\/span><\/em><span>\u00a0\u00e9 a quantidade de subst\u00e2ncia<\/span><\/li>\n<li><em><span>T<\/span><\/em><span>\u00a0\u00e9 a temperatura absoluta<\/span><\/li>\n<li><em><span>V<\/span><\/em><span>\u00a0\u00e9 o volume<\/span><\/li>\n<li><em><span>R<\/span><\/em><span>\u00a0\u00a0\u00e9 a constante de g\u00e1s ideal, ou universal, igual ao produto da constante de Boltzmann e da constante de Avogadro,<\/span><\/li>\n<\/ul>\n<p><span>Nesta equa\u00e7\u00e3o, o s\u00edmbolo R \u00e9 uma constante chamada constante universal de g\u00e1s que tem o mesmo valor para todos os gases &#8211; ou seja, R = 8,31 J \/ mol K.<\/span><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-40 lgc-tablet-grid-40 lgc-mobile-grid-100 lgc-equal-heights  lgc-last\">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17321\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17321\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Guy-Lussac-Law.png\"><img loading=\"lazy\" class=\"wp-image-17321 size-full lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Guy-Lussac-Law.png\" alt=\"Lei de Guy-Lussac\" width=\"274\" height=\"301\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Guy-Lussac-Law.png\" \/><\/a><figcaption id=\"caption-attachment-17321\" class=\"wp-caption-text\"><span>Para uma massa fixa de g\u00e1s em volume constante, a press\u00e3o \u00e9 diretamente proporcional \u00e0 temperatura Kelvin.\u00a0Fonte: grc.nasa.gov A pol\u00edtica de direitos autorais da NASA afirma que \u201co material da NASA n\u00e3o \u00e9 protegido por direitos autorais, a menos que seja observado\u201d.<\/span><\/figcaption><\/figure>\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>Lei de Avogadro<\/span><\/h2>\n<p><strong><span>A lei de Avogadro<\/span><\/strong><span>\u00a0\u00e9 uma das leis de g\u00e1s.\u00a0No in\u00edcio do s\u00e9culo XIX, um cientista italiano\u00a0<\/span><strong><span>Lorenzo Romano Amedeo Carlo Avogadro<\/span><\/strong><span>\u00a0estudou a rela\u00e7\u00e3o entre o\u00a0<\/span><strong><span>volume<\/span><\/strong><span>\u00a0\u00a0e a\u00a0<\/span><strong><span>quantidade<\/span><\/strong><span>\u00a0de subst\u00e2ncia presente no g\u00e1s.\u00a0Os resultados de certas experi\u00eancias com gases o levaram a formular uma conhecida\u00a0<\/span><strong><span>Lei de Avogadro<\/span><\/strong><span>\u00a0.\u00a0Afirma que, nas mesmas condi\u00e7\u00f5es de temperatura e press\u00e3o, volumes iguais de gases diferentes cont\u00eam um n\u00famero igual de mol\u00e9culas, ou:<\/span><\/p>\n<p><em><span>Para uma massa fixa de um g\u00e1s ideal a press\u00e3o e temperatura constantes, o volume e a quantidade do g\u00e1s s\u00e3o diretamente proporcionais.<\/span><\/em><\/p>\n<p><span>Voc\u00ea pode expressar isso matematicamente como:<\/span><\/p>\n<p><strong><em><span>V\u00a0<\/span><\/em><em><span>\u221d\u00a0<\/span><\/em><em><span>n<\/span><\/em><\/strong><\/p>\n<p><span>ou<\/span><\/p>\n<p><strong><em><span>V = constante.\u00a0n<\/span><\/em><\/strong><\/p>\n<p><span>onde nR \/ V \u00e9 constante e:<\/span><\/p>\n<ul>\n<li><em><span>n<\/span><\/em><span>\u00a0\u00e9 a quantidade de subst\u00e2ncia medida em moles<\/span><\/li>\n<li><em><span>V<\/span><\/em><span>\u00a0\u00e9 o volume do g\u00e1s<\/span><\/li>\n<\/ul>\n<p><span>a constante \u00e9 igual a RT \/ p, onde\u00a0<\/span><em><span>p<\/span><\/em><span>\u00a0\u00e9 a press\u00e3o absoluta do g\u00e1s,\u00a0<\/span><em><span>T<\/span><\/em><span>\u00a0\u00e9 a temperatura absoluta e\u00a0<\/span><em><span>R<\/span><\/em><span>\u00a0\u00a0\u00e9 a constante de g\u00e1s ideal, ou universal, igual ao produto da constante de Boltzmann e da constante de Avogadro.<\/span><\/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>N\u00famero de Avogadro<\/span><\/h2>\n<p><span>Em homenagem a\u00a0<\/span><strong><span>Avogadro<\/span><\/strong><span>\u00a0, tamb\u00e9m o n\u00famero de part\u00edculas (\u00e1tomos, mol\u00e9culas, \u00edons ou outras part\u00edculas) em\u00a0<\/span><strong><span>1 mole<\/span><\/strong><span>\u00a0de uma subst\u00e2ncia,\u00a0<\/span><strong><span>6.022 \u00d7 10\u00a0<\/span><sup><span>23<\/span><\/sup><\/strong><span>\u00a0, recebeu o nome de Avogadro como\u00a0<\/span><strong><span>constante de\u00a0<\/span><\/strong><strong><span>Avogadro<\/span><\/strong><span>\u00a0ou\u00a0<strong>n\u00famero de Avogadro<\/strong>\u00a0.\u00a0A constante de Avogadro \u00e9 uma das unidades de base SI sete e representado por\u00a0<\/span><em><span>N\u00a0<\/span><\/em><sub><span>A<\/span><\/sub><span>\u00a0.<\/span><\/p>\n<p><span>A\u00a0<\/span><strong><span>Lei de Avogadro<\/span><\/strong><span>\u00a0pode ser usada para comparar a mesma subst\u00e2ncia sob dois conjuntos diferentes de condi\u00e7\u00f5es:<\/span><\/p>\n<p><strong><em><span>V\u00a0<\/span><\/em><em><sub><span>1<\/span><\/sub><\/em><em><span>\u00a0\/ n\u00a0<\/span><\/em><em><sub><span>1<\/span><\/sub><\/em><em><span>\u00a0= V\u00a0<\/span><\/em><em><sub><span>2<\/span><\/sub><\/em><em><span>\u00a0\/ n\u00a0<\/span><\/em><em><sub><span>2<\/span><\/sub><\/em><\/strong><\/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>Volume molar de gases<\/span><\/h2>\n<p><span>Um dos resultados mais pr\u00e1ticos desta lei \u00e9 o\u00a0<\/span><strong><span>volume molar de um g\u00e1s<\/span><\/strong><span>\u00a0,\u00a0<\/span><strong><span>V\u00a0<\/span><sub><span>m<\/span><\/sub><\/strong><span>\u00a0, que \u00e9 sobre:<\/span><\/p>\n<p><strong><span>V\u00a0<\/span><sub><span>m<\/span><\/sub><span>\u00a0= 22,4 dm\u00a0<\/span><sup><span>3<\/span><\/sup><span>\u00a0\/ mol<\/span><\/strong><\/p>\n<p><span>Isso significa que, \u00e0 temperatura padr\u00e3o (273,15 K, 0 \u00b0 C) e\u00a0<\/span><a title=\"Press\u00e3o atmosf\u00e9rica\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-pressure-physics\/atmospheric-pressure\/\"><span>press\u00e3o atmosf\u00e9rica<\/span><\/a><span>\u00a0padr\u00e3o\u00a0(101,325 kPa), o volume molar \u00e9 o mesmo para todos os gases ideais.\u00a0Observe que est\u00e1 sob a hip\u00f3tese ideal de g\u00e1s.\u00a0Este valor \u00e9 fortemente dependente da press\u00e3o e da temperatura.\u00a0Por exemplo:<\/span><\/p>\n<ul>\n<li><span>para 273,15 K (0 \u00b0 C) e 100,00 kPa, o volume molar de um g\u00e1s ideal \u00e9 22,71 dm\u00a0<\/span><sup><span>3<\/span><\/sup><span>\u00a0.mol\u00a0<\/span><sup><span>\u22121<\/span><\/sup><span>\u00a0.<\/span><\/li>\n<li><span>para 298,15 K (25 \u00b0 C) e 100,00 kPa, o volume molar de um g\u00e1s ideal \u00e9 24,79 dm\u00a0<\/span><sup><span>3<\/span><\/sup><span>\u00a0.mol\u00a0<\/span><sup><span>\u22121<\/span><\/sup><span>\u00a0.<\/span><\/li>\n<\/ul>\n<\/div>\n<\/div>\n<p>&nbsp;<\/p>\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<\/div>\n<\/div>\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>Em geral, as leis dos gases s\u00e3o as primeiras equa\u00e7\u00f5es de estado, que correlacionam densidades de gases e l\u00edquidos a temperaturas e press\u00f5es.\u00a0As leis de g\u00e1s foram completamente desenvolvidas no final do s\u00e9culo XVIII.\u00a0Engenharia T\u00e9rmica Leis do g\u00e1s Em geral, as\u00a0leis\u00a0dos\u00a0gases\u00a0s\u00e3o as\u00a0primeiras\u00a0equa\u00e7\u00f5es de estado\u00a0, que correlacionam densidades de gases e l\u00edquidos a temperaturas e press\u00f5es.\u00a0As\u00a0leis &#8230; <a title=\"O que \u00e9 a lei dos gases &#8211; Defini\u00e7\u00e3o\" class=\"read-more\" href=\"https:\/\/www.thermal-engineering.org\/pt-br\/o-que-e-a-lei-dos-gases-definicao\/\" aria-label=\"More on O que \u00e9 a lei dos gases &#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 a lei dos gases - Defini\u00e7\u00e3o<\/title>\n<meta name=\"description\" content=\"Em geral, as leis dos gases s\u00e3o as primeiras equa\u00e7\u00f5es de estado, que correlacionam densidades de gases e l\u00edquidos a temperaturas e press\u00f5es. 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