{"id":52453,"date":"2020-02-19T13:58:44","date_gmt":"2020-02-19T12:58:44","guid":{"rendered":"https:\/\/www.thermal-engineering.org\/quest-ce-quun-cycle-double-cycle-de-pression-limite-definition\/"},"modified":"2021-05-28T10:44:17","modified_gmt":"2021-05-28T09:44:17","slug":"quest-ce-quun-cycle-double-cycle-de-pression-limite-definition","status":"publish","type":"post","link":"https:\/\/www.thermal-engineering.org\/fr\/quest-ce-quun-cycle-double-cycle-de-pression-limite-definition\/","title":{"rendered":"Qu&#8217;est-ce qu&#8217;un Cycle de Sabath\u00e9 &#8211; D\u00e9finition"},"content":{"rendered":"<div class=\"su-quote su-quote-style-default\">\n<div class=\"su-quote-inner su-clearfix\">Le Cycle de Sabath\u00e9, ou cycle de pression limit\u00e9, est un cycle thermodynamique qui combine le cycle Otto et le cycle Diesel. Un cycle double comprend cinq processus thermodynamiques. G\u00e9nie thermique<\/div>\n<\/div>\n<div class=\"su-divider su-divider-style-dotted\"><\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-50 lgc-tablet-grid-50 lgc-mobile-grid-100 lgc-equal-heights lgc-first\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>Cycle diesel &#8211; moteur diesel<\/h2>\n<p><strong>Le cycle double<\/strong>\u00a0, ou\u00a0<strong>cycle de pression limit\u00e9<\/strong>\u00a0, est un\u00a0<strong>cycle thermodynamique<\/strong>\u00a0qui combine le\u00a0<a title=\"Cycle Otto - Moteur Otto\" href=\"https:\/\/www.thermal-engineering.org\/what-is-otto-cycle-otto-engine-definition\/\"><strong>cycle Otto<\/strong><\/a>\u00a0et le\u00a0<a title=\"Cycle diesel - moteur diesel\" href=\"https:\/\/www.thermal-engineering.org\/what-is-diesel-cycle-diesel-engine-definition\/\"><strong>cycle Diesel<\/strong><\/a>\u00a0.\u00a0Dans le cycle double, la combustion se produit en partie \u00e0 volume constant et en partie \u00e0 pression constante.\u00a0Il peut \u00eatre utilis\u00e9 pour d\u00e9crire les moteurs \u00e0 combustion interne.\u00a0Les diagrammes pression-volume des moteurs \u00e0 combustion interne actuels ne sont pas bien d\u00e9crits par les cycles Otto et Diesel.\u00a0Un cycle air standard qui peut \u00eatre rapproch\u00e9 des variations de pression est le cycle double air.\u00a0Une approche plus efficace consisterait \u00e0 mod\u00e9liser le processus de combustion des moteurs Otto et Diesel en combinant deux processus de transfert de chaleur, un\u00a0<a title=\"Processus isochorique - Processus isom\u00e9trique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-isochoric-process-isometric-process-definition\/\"><strong>processus isochore<\/strong><\/a>\u00a0et un<a title=\"Processus isobare\" href=\"https:\/\/www.thermal-engineering.org\/what-is-isobaric-process-definition\/\"><strong>processus isobare<\/strong><\/a>\u00a0.<\/p>\n<p>Par rapport \u00e0 un cycle Otto, qui suppose une addition de chaleur instantan\u00e9e (une addition de chaleur isochore), dans un\u00a0<strong>cycle double, de la<\/strong>\u00a0chaleur est ajout\u00e9e partiellement \u00e0 volume constant et partiellement \u00e0 pression constante.\u00a0Par cons\u00e9quent, l&#8217;avantage est qu&#8217;il reste plus de temps pour que le combustible br\u00fble compl\u00e8tement.\u00a0D&#8217;autre part, l&#8217;utilisation d&#8217;un cycle double est\u00a0<strong>l\u00e9g\u00e8rement plus complexe<\/strong>\u00a0.\u00a0L&#8217;efficacit\u00e9 thermique se situe entre les cycles Otto et Diesel.<\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-50 lgc-tablet-grid-50 lgc-mobile-grid-100 lgc-equal-heights lgc-last\">\n<div class=\"inside-grid-column\">\n<p><strong>Le cycle double combine le cycle Otto et le cycle Diesel.\u00a0<\/strong>.\u00a0Sur cette image, il y a un moteur Otto, qui est allum\u00e9 par une bougie \u00e0 la place de la compression.<\/p>\n<figure id=\"attachment_17548\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17548\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Four-Stroke-Engine-Otto-Engine.gif\"><img loading=\"lazy\" class=\"size-full wp-image-17548 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Four-Stroke-Engine-Otto-Engine.gif\" alt=\"Moteur quatre temps - Moteur Otto\" width=\"225\" height=\"300\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Four-Stroke-Engine-Otto-Engine.gif\" \/><\/a><figcaption id=\"caption-attachment-17548\" class=\"wp-caption-text\">Moteur \u00e0 quatre temps &#8211; Moteur Otto<br \/>\nSource: wikipedia.org, oeuvre de Zephyris, CC BY-SA 3.0<\/figcaption><\/figure>\n<div class=\"su-youtube su-responsive-media-yes\"><iframe class=\"lazy-loaded\" src=\"https:\/\/www.youtube.com\/embed\/xflY5uS-nnw?\" width=\"340\" height=\"200\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-lazy-type=\"iframe\" data-src=\"https:\/\/www.youtube.com\/embed\/xflY5uS-nnw?\" data-mce-fragment=\"1\"><\/iframe><\/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<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>Cycle de Sabath\u00e9 &#8211; Processus<\/h2>\n<p>Dans un\u00a0<strong>cycle double<\/strong>\u00a0, le syst\u00e8me ex\u00e9cutant le cycle subit une s\u00e9rie de cinq processus: deux processus isentropiques (adiabatiques r\u00e9versibles) altern\u00e9s avec deux processus isochoriques et un processus isobare:<\/p>\n<ul>\n<li>\n<figure id=\"attachment_17668\" class=\"wp-caption alignright\" aria-describedby=\"caption-attachment-17668\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-Cycle-Mixed-Cycle-pV-Diagram.png\"><img loading=\"lazy\" class=\"size-medium wp-image-17668 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-Cycle-Mixed-Cycle-pV-Diagram-300x277.png\" alt=\"Double cycle - Diagramme pV\" width=\"300\" height=\"277\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-Cycle-Mixed-Cycle-pV-Diagram-300x277.png\" \/><\/a><figcaption id=\"caption-attachment-17668\" class=\"wp-caption-text\">Double cycle &#8211; Diagramme pV<\/figcaption><\/figure>\n<p><strong>Compression isentropique<\/strong>\u00a0(course de compression) &#8211; Le gaz est comprim\u00e9 de mani\u00e8re adiabatique de l&#8217;\u00e9tat 1 \u00e0 l&#8217;\u00e9tat 2, lorsque le piston se d\u00e9place du point de fermeture de la soupape d&#8217;admission (1) au point mort haut.\u00a0Les environs agissent sur le gaz, augmentant son \u00e9nergie interne (temp\u00e9rature) et le compressant.\u00a0En revanche, l&#8217;entropie reste inchang\u00e9e.\u00a0L&#8217;\u00e9volution des volumes et de son rapport (\u00a0<em>V\u00a0<\/em><em><sub>1<\/sub><\/em><em>\u00a0\/ V\u00a0<\/em><em><sub>2<\/sub><\/em>\u00a0) est connue sous le nom de taux de compression.\u00a0Le taux de compression est inf\u00e9rieur au taux d&#8217;expansion.<\/li>\n<li><strong>Compression isochore<\/strong>\u00a0(phase d&#8217;allumage) &#8211; Dans cette phase (entre l&#8217;\u00e9tat 2 et l&#8217;\u00e9tat 3), il y a un transfert de chaleur \u00e0 volume constant (le piston est au repos) vers l&#8217;air \u00e0 partir d&#8217;une source externe tandis que le piston est au repos au point mort haut .\u00a0Ce processus est similaire au processus isochore du cycle d&#8217;Otto.\u00a0Il est destin\u00e9 \u00e0 repr\u00e9senter l&#8217;inflammation du m\u00e9lange carburant-air inject\u00e9 dans la chambre et la combustion rapide qui en r\u00e9sulte.\u00a0La pression augmente et le rapport (\u00a0<em>P\u00a0<\/em><em><sub>3<\/sub><\/em><em>\u00a0\/ P\u00a0<\/em><em><sub>2<\/sub><\/em>\u00a0) est appel\u00e9 \u00abrapport d&#8217;explosion\u00bb.<\/li>\n<li><strong>Expansion isobare<\/strong>\u00a0(course motrice) &#8211; Dans cette phase (entre l&#8217;\u00e9tat 3 et l&#8217;\u00e9tat 4), il y a un transfert de chaleur \u00e0 pression constante (mod\u00e8le id\u00e9alis\u00e9) vers l&#8217;air \u00e0 partir d&#8217;une source externe (combustion du carburant) tandis que le piston se d\u00e9place vers le V\u00a0<sub>4<\/sub>\u00a0.\u00a0Pendant le processus \u00e0 pression constante, l&#8217;\u00e9nergie p\u00e9n\u00e8tre dans le syst\u00e8me sous forme de chaleur Q\u00a0<sub>ajout\u00e9e<\/sub>\u00a0, et une partie du travail se fait en d\u00e9pla\u00e7ant le piston.<\/li>\n<li><strong>Expansion isentropique<\/strong>\u00a0(course de puissance) &#8211; Le gaz se d\u00e9tend adiabatiquement de l&#8217;\u00e9tat 4 \u00e0 l&#8217;\u00e9tat 5, lorsque le piston se d\u00e9place de V\u00a0<sub>3<\/sub>\u00a0au point mort bas.\u00a0Le gaz travaille sur l&#8217;environnement (piston) et perd une quantit\u00e9 d&#8217;\u00e9nergie interne \u00e9gale au travail qui quitte le syst\u00e8me.\u00a0Encore une fois, l&#8217;entropie reste inchang\u00e9e.<\/li>\n<li><strong>D\u00e9compression isochore (course d&#8217;\u00e9chappement)<\/strong>\u00a0&#8211; Dans cette phase, le cycle se termine par un processus \u00e0 volume constant dans lequel la chaleur est rejet\u00e9e de l&#8217;air tandis que le piston est au point mort bas.\u00a0La pression du gaz de travail chute instantan\u00e9ment du point 5 au point 1. La soupape d&#8217;\u00e9chappement s&#8217;ouvre au point 5. La course d&#8217;\u00e9chappement est directement apr\u00e8s cette d\u00e9compression.\u00a0Lorsque le piston se d\u00e9place du point mort bas (point 1) au point mort haut (point 0) avec la soupape d&#8217;\u00e9chappement ouverte, le m\u00e9lange gazeux est \u00e9vacu\u00e9 vers l&#8217;atmosph\u00e8re et le processus recommence.<\/li>\n<\/ul>\n<p>Pendant le cycle double, le travail est effectu\u00e9 sur le gaz par le piston entre les \u00e9tats 1 et 2 (\u00a0<strong>i\u00a0<\/strong><strong>compression sentropique<\/strong>\u00a0).\u00a0Le travail se fait par le gaz sur le piston entre les \u00e9tapes 2 et 3 (\u00a0<strong>i\u00a0<\/strong><strong>addition de chaleur sobarique<\/strong>\u00a0) et entre les \u00e9tapes 2 et 3 (\u00a0<strong>i\u00a0<\/strong><strong>expansion sentropique<\/strong>\u00a0).\u00a0La diff\u00e9rence entre le travail effectu\u00e9 par le gaz et le travail effectu\u00e9 sur le gaz est le travail net produit par le cycle et il correspond \u00e0 la zone d\u00e9limit\u00e9e par la courbe du cycle.\u00a0Le travail produit par le cycle multiplie la vitesse du cycle (cycles par seconde) par la puissance produite par le moteur Diesel.<\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights lgc-first\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>Processus isentropique<\/h2>\n<p>Un\u00a0<a title=\"Processus isentropique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-isentropic-process-definition\/\"><strong>processus isentropique<\/strong><\/a>\u00a0est un\u00a0<a title=\"Processus thermodynamiques\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermodynamic-process-definition\/\"><strong>processus thermodynamique<\/strong><\/a>\u00a0, dans lequel l&#8217;\u00a0<a title=\"Qu'est-ce que l'entropie\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/what-is-entropy\/\"><strong>entropie<\/strong>\u00a0<\/a>du fluide ou du gaz reste constante.\u00a0Cela signifie que le\u00a0<strong>processus isentropique<\/strong>\u00a0est un cas particulier d&#8217;un\u00a0<strong>processus adiabatique<\/strong>\u00a0dans lequel il n&#8217;y a pas de transfert de chaleur ou de mati\u00e8re.\u00a0Il s&#8217;agit d&#8217;un\u00a0<strong>processus adiabatique r\u00e9versible<\/strong>\u00a0.\u00a0L&#8217;hypoth\u00e8se d&#8217;absence de transfert de chaleur est tr\u00e8s importante, car nous ne pouvons utiliser l&#8217;approximation adiabatique que dans\u00a0<strong>des processus tr\u00e8s rapides<\/strong>\u00a0.<\/p>\n<p><strong>Processus isentropique et premi\u00e8re loi<\/strong><\/p>\n<p>Pour un syst\u00e8me ferm\u00e9, on peut \u00e9crire la\u00a0<strong><a title=\"Premi\u00e8re loi en termes d'enthalpie 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\/\">premi\u00e8re loi de la thermodynamique en termes d&#8217;enthalpie<\/a><\/strong>\u00a0:<\/p>\n<p><strong>dH = dQ + Vdp<\/strong><\/p>\n<p><strong>ou<\/strong><\/p>\n<p><strong>dH = TdS + Vdp<\/strong><\/p>\n<p><strong>Processus isentropique (dQ = 0):<\/strong><\/p>\n<p><strong>dH = Vdp \u2192 W = H\u00a0<\/strong><strong><sub>2<\/sub><\/strong><strong>\u00a0&#8211; H\u00a0<\/strong><strong><sub>1<\/sub><\/strong><strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u2192 H\u00a0<\/strong><strong><sub>2<\/sub><\/strong><strong>\u00a0&#8211; H\u00a0<\/strong><strong><sub>1<\/sub><\/strong><strong>\u00a0=\u00a0<em>C\u00a0<\/em><\/strong><strong><em><sub>p<\/sub><\/em><\/strong><strong><em>\u00a0(T\u00a0<\/em><\/strong><strong><em><sub>2<\/sub><\/em><\/strong><strong><em>\u00a0&#8211; T\u00a0<\/em><\/strong><strong><em><sub>1<\/sub><\/em><\/strong><strong><em>\u00a0) \u00a0\u00a0\u00a0<\/em><\/strong><em>\u00a0(pour\u00a0<a title=\"Qu'est-ce que le gaz id\u00e9al\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/ideal-gas-law\/what-is-ideal-gas\/\">le gaz id\u00e9al<\/a>\u00a0)<\/em><\/p>\n<p><strong>Processus isentropique du gaz id\u00e9al<\/strong><\/p>\n<p>Le\u00a0<strong>processus isentropique<\/strong>\u00a0(un cas particulier du processus adiabatique) peut \u00eatre exprim\u00e9 avec la\u00a0<a title=\"Loi du gaz id\u00e9al\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/ideal-gas-law\/\"><strong>loi du gaz id\u00e9al<\/strong><\/a>\u00a0comme:<\/p>\n<p><strong><em>pV\u00a0<sup>\u03ba<\/sup>\u00a0= constant<\/em><\/strong><\/p>\n<p>ou<\/p>\n<p><em><strong>p\u00a0<sub>1<\/sub>\u00a0V\u00a0<sub>1\u00a0<\/sub><sup>\u03ba<\/sup>\u00a0= p\u00a0<sub>2<\/sub>\u00a0V\u00a0<sub>2\u00a0<\/sub><sup>\u03ba<\/sup><\/strong><\/em><\/p>\n<p>dans laquelle\u00a0<strong>\u03ba = c\u00a0<sub>p<\/sub>\u00a0\/ c\u00a0<sub>v<\/sub><\/strong>\u00a0est le rapport des\u00a0<a title=\"Capacit\u00e9 calorifique - Capacit\u00e9 calorifique sp\u00e9cifique\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/heat-capacity\/\"><strong>chaleurs sp\u00e9cifiques<\/strong><\/a>\u00a0(ou\u00a0<strong>capacit\u00e9s calorifiques<\/strong>\u00a0) pour le gaz.\u00a0Un pour\u00a0<strong>une pression constante (c\u00a0<\/strong><strong><sub>p<\/sub><\/strong><strong>\u00a0)<\/strong>\u00a0et un pour\u00a0<strong>un volume constant (c\u00a0<\/strong><strong><sub>v<\/sub><\/strong><strong>\u00a0)<\/strong>\u00a0.\u00a0Notez que ce rapport\u00a0<strong>\u03ba\u00a0\u00a0<\/strong><strong>= c\u00a0<\/strong><strong><sub>p<\/sub><\/strong><strong>\u00a0\/ c\u00a0<\/strong><strong><sub>v<\/sub><\/strong>\u00a0est un facteur d\u00e9terminant la vitesse du son dans un gaz et d&#8217;autres processus adiabatiques.<\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights \">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>Processus isochorique<\/h2>\n<p>Un\u00a0<a title=\"Processus isochorique - Processus isom\u00e9trique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-isochoric-process-isometric-process-definition\/\"><strong>processus isochore<\/strong><\/a>\u00a0est un processus thermodynamique, dans lequel le\u00a0<strong>volume<\/strong>\u00a0du syst\u00e8me ferm\u00e9\u00a0<strong>reste constant<\/strong>\u00a0(V = const).\u00a0Il d\u00e9crit le comportement du gaz \u00e0 l&#8217;int\u00e9rieur du conteneur, qui ne peut pas \u00eatre d\u00e9form\u00e9.\u00a0\u00c9tant donn\u00e9 que le volume reste constant, le transfert de chaleur dans ou hors du syst\u00e8me ne fonctionne pas avec le\u00a0<a title=\"Travaux p\u0394V - Travaux aux limites et travaux V\u0394p\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/p%ce%b4v-work-boundary-work-and-v%ce%b4p-work\/\">p\u2206V<\/a>\u00a0, mais modifie uniquement l&#8217;\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-internal-energy-thermal-energy-definition\/\"><strong>\u00e9nergie interne<\/strong><\/a>\u00a0(la temp\u00e9rature) du syst\u00e8me.<\/p>\n<p><strong>Processus isochorique et premi\u00e8re loi<\/strong><\/p>\n<p>La forme classique de la\u00a0<a title=\"Premi\u00e8re loi de la thermodynamique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-first-law-of-thermodynamics-definition\/\">premi\u00e8re loi de la thermodynamique<\/a>\u00a0est l&#8217;\u00e9quation suivante:<\/p>\n<p><strong>dU = dQ &#8211; dW<\/strong><\/p>\n<p>Dans cette \u00e9quation, dW est \u00e9gal \u00e0\u00a0<strong>dW = pdV<\/strong>\u00a0et est connu comme le\u00a0<a title=\"Travaux p\u0394V - Travaux aux limites et travaux V\u0394p\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/p%ce%b4v-work-boundary-work-and-v%ce%b4p-work\/\">travail<\/a>\u00a0aux\u00a0<a title=\"Travaux p\u0394V - Travaux aux limites et travaux V\u0394p\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/p%ce%b4v-work-boundary-work-and-v%ce%b4p-work\/\">limites<\/a>\u00a0.\u00a0Alors:<\/p>\n<p><strong>dU = dQ &#8211; pdV<\/strong><\/p>\n<p>Dans le\u00a0<strong>processus isochore<\/strong>\u00a0et le\u00a0<strong>gaz id\u00e9al<\/strong>\u00a0, toute la chaleur ajout\u00e9e au syst\u00e8me sera utilis\u00e9e pour augmenter l&#8217;\u00e9nergie interne.<\/p>\n<p><strong>Processus isochorique (pdV = 0):<\/strong><\/p>\n<p><strong>dU = dQ \u00a0\u00a0\u00a0\u00a0<\/strong><em>(pour le gaz id\u00e9al)<\/em><\/p>\n<p><strong>dU = 0 = Q &#8211; W \u2192 W = Q \u00a0\u00a0<em>\u00a0\u00a0\u00a0\u00a0<\/em><\/strong><em>(pour le gaz id\u00e9al)<\/em><\/p>\n<p><strong>Processus isochorique du gaz id\u00e9al<\/strong><\/p>\n<p>Le\u00a0<strong>processus isochore<\/strong>\u00a0peut s&#8217;exprimer avec la\u00a0<a title=\"Loi du gaz id\u00e9al\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/ideal-gas-law\/\"><strong>loi du gaz id\u00e9al<\/strong><\/a>\u00a0comme:<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-1.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-17465 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-1.png\" alt=\"processus isochore - \u00e9quation 1\" width=\"138\" height=\"52\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-1.png\" \/><\/a><\/p>\n<p>ou<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-2.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-17466 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-2.png\" alt=\"processus isochore - \u00e9quation 2\" width=\"86\" height=\"66\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isochoric-process-equation-2.png\" \/><\/a><\/p>\n<p>Sur un\u00a0<strong>diagramme pV<\/strong>\u00a0, le processus se produit le long d&#8217;une ligne horizontale qui a l&#8217;\u00e9quation V = constante.<\/p>\n<p>Voir aussi:\u00a0\u00a0<a title=\"Loi de Guy-Lussac\" href=\"https:\/\/www.thermal-engineering.org\/what-is-guy-lussacs-law-definition\/\">Loi de Guy-Lussac<\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>Processus isobare<\/h2>\n<p>Un\u00a0<strong>processus isobare<\/strong>\u00a0est un\u00a0<a title=\"Processus thermodynamiques\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermodynamic-process-definition\/\">processus thermodynamique<\/a>\u00a0, dans lequel la\u00a0<a title=\"Qu'est-ce que la pression - Physique\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-pressure-physics\/\"><strong>pression<\/strong><\/a>\u00a0du syst\u00e8me\u00a0<strong>reste constante<\/strong>\u00a0(p = const).\u00a0Le transfert de chaleur dans ou hors du syst\u00e8me fonctionne, mais modifie \u00e9galement l&#8217;\u00e9nergie interne du syst\u00e8me.<\/p>\n<p>Puisqu&#8217;il y a des changements d&#8217;\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-internal-energy-thermal-energy-definition\/\">\u00e9nergie interne<\/a>\u00a0(dU) et des changements de volume du syst\u00e8me (\u2206V), les ing\u00e9nieurs utilisent souvent l&#8217;\u00a0<a title=\"Qu'est-ce que l'enthalpie\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/what-is-enthalpy\/\"><strong>enthalpie<\/strong><\/a>\u00a0du syst\u00e8me, qui est d\u00e9finie comme:<\/p>\n<p><em><strong>H = U + pV<\/strong><\/em><\/p>\n<p><strong>Processus isobare et premi\u00e8re loi<\/strong><\/p>\n<p>La forme classique de la\u00a0<a title=\"Premi\u00e8re loi de la thermodynamique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-first-law-of-thermodynamics-definition\/\">premi\u00e8re loi de la thermodynamique<\/a>\u00a0est l&#8217;\u00e9quation suivante:<\/p>\n<p><strong>dU = dQ &#8211; dW<\/strong><\/p>\n<p>Dans cette \u00e9quation, dW est \u00e9gal \u00e0\u00a0<strong>dW = pdV<\/strong>\u00a0et est connu comme le\u00a0<a title=\"Travaux p\u0394V - Travaux aux limites et travaux V\u0394p\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/p%ce%b4v-work-boundary-work-and-v%ce%b4p-work\/\">travail<\/a>\u00a0aux\u00a0<a title=\"Travaux p\u0394V - Travaux aux limites et travaux V\u0394p\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/laws-of-thermodynamics\/first-law-of-thermodynamics\/p%ce%b4v-work-boundary-work-and-v%ce%b4p-work\/\">limites<\/a>\u00a0.\u00a0Dans un proc\u00e9d\u00e9 isobare et le gaz id\u00e9al, une\u00a0<strong>partie de la chaleur ajout\u00e9e<\/strong>\u00a0au syst\u00e8me sera utilis\u00e9e pour\u00a0<strong>faire le travail<\/strong>\u00a0et une\u00a0<strong>partie de la chaleur<\/strong>\u00a0ajout\u00e9e augmentera l&#8217;\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-internal-energy-thermal-energy-definition\/\"><strong>\u00e9nergie interne<\/strong><\/a>\u00a0(augmentera la temp\u00e9rature).\u00a0Par cons\u00e9quent, il est commode d&#8217;utiliser l&#8217;\u00a0<strong>enthalpie<\/strong>\u00a0au lieu de l&#8217;\u00e9nergie interne.<\/p>\n<p><strong>Processus isobare (Vdp = 0):<\/strong><\/p>\n<p><strong>dH = dQ \u2192 Q = H\u00a0<\/strong><strong><sub>2<\/sub><\/strong><strong>\u00a0&#8211; H\u00a0<\/strong><strong><sub>1<\/sub><\/strong><\/p>\n<p><strong>\u00c0 entropie constante<\/strong>\u00a0, c&#8217;est-\u00e0-dire dans un processus isentropique, le\u00a0<strong>changement d&#8217;enthalpie<\/strong>\u00a0est \u00e9gal au\u00a0<strong>travail de processus d&#8217;\u00e9coulement<\/strong>\u00a0effectu\u00e9 sur ou par le syst\u00e8me.<\/p>\n<p><strong>Processus isobare du gaz id\u00e9al<\/strong><\/p>\n<p>Le\u00a0<strong>processus isobare<\/strong>\u00a0peut s&#8217;exprimer avec la\u00a0<a title=\"Loi du gaz id\u00e9al\" href=\"https:\/\/www.nuclear-power.com\/nuclear-engineering\/thermodynamics\/ideal-gas-law\/\"><strong>loi du gaz id\u00e9al<\/strong><\/a>\u00a0comme:<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-2.png?a34b7f\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-17430 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-2.png?a34b7f\" alt=\"processus isobare - \u00e9quation - 2\" width=\"134\" height=\"63\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-2.png?a34b7f\" \/><\/a><\/p>\n<p>ou<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-3.png?a34b7f\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-17431 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-3.png?a34b7f\" alt=\"processus isobare - \u00e9quation - 3\" width=\"77\" height=\"67\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/isobaric-process-equation-3.png?a34b7f\" \/><\/a><\/p>\n<p>Sur un\u00a0<strong>diagramme pV<\/strong>\u00a0, le processus se produit le long d&#8217;une ligne horizontale (appel\u00e9e isobare) qui a l&#8217;\u00e9quation p = constante.<\/p>\n<p>Voir aussi:\u00a0<a title=\"La loi de Charles\" href=\"https:\/\/www.thermal-engineering.org\/what-is-charless-law-definition\/\">Charles&#8217;s Law<\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights lgc-first\">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17280\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17280\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isentropic-Process-characteristics.png\"><img loading=\"lazy\" class=\"size-full wp-image-17280 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isentropic-Process-characteristics.png\" alt=\"Processus isentropique - caract\u00e9ristiques\" width=\"386\" height=\"609\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isentropic-Process-characteristics.png\" \/><\/a><figcaption id=\"caption-attachment-17280\" class=\"wp-caption-text\">Processus isentropique &#8211; principales caract\u00e9ristiques<\/figcaption><\/figure>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights \">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17463\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17463\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isochoric-process-main-characteristics.png\"><img loading=\"lazy\" class=\"size-full wp-image-17463 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isochoric-process-main-characteristics.png\" alt=\"Processus isochorique - principales caract\u00e9ristiques\" width=\"382\" height=\"468\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isochoric-process-main-characteristics.png\" \/><\/a><figcaption id=\"caption-attachment-17463\" class=\"wp-caption-text\">Processus isochorique &#8211; principales caract\u00e9ristiques<\/figcaption><\/figure>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights lgc-last\">\n<div class=\"inside-grid-column\">\n<figure id=\"attachment_17426\" class=\"wp-caption aligncenter\" aria-describedby=\"caption-attachment-17426\"><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isobaric-process-main-characteristics.png\"><img loading=\"lazy\" class=\"size-full wp-image-17426 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isobaric-process-main-characteristics.png\" alt=\"Processus isobare - principales caract\u00e9ristiques\" width=\"381\" height=\"717\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Isobaric-process-main-characteristics.png\" \/><\/a><figcaption id=\"caption-attachment-17426\" class=\"wp-caption-text\">Processus isobare &#8211; principales caract\u00e9ristiques<\/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>Efficacit\u00e9 thermique pour double cycle<\/h2>\n<p>En g\u00e9n\u00e9ral ,\u00a0le\u00a0<a title=\"Efficacit\u00e9 thermique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermal-efficiency-definition\/\"><strong>rendement thermique<\/strong><\/a><a title=\"Efficacit\u00e9 thermique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermal-efficiency-definition\/\">\u00a0,\u00a0<\/a><a title=\"Efficacit\u00e9 thermique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermal-efficiency-definition\/\"><strong><em>\u03b7\u00a0<\/em><\/strong><\/a><a title=\"Efficacit\u00e9 thermique\" href=\"https:\/\/www.thermal-engineering.org\/what-is-thermal-efficiency-definition\/\"><strong><em><sub>e<\/sub><\/em><\/strong><\/a>\u00a0, d&#8217;un moteur thermique est d\u00e9finie comme \u00e9tant le rapport entre le\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-work-in-thermodynamics-definition\/\">travail<\/a>\u00a0qu&#8217;elle fait,\u00a0<strong>W<\/strong>\u00a0, \u00e0 la\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-heat-in-physics-heat-definition\/\">chaleur<\/a>\u00a0d&#8217; entr\u00e9e \u00e0 la temp\u00e9rature \u00e9lev\u00e9e, 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=\"formule d'efficacit\u00e9 thermique - 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>L&#8217;\u00a0<strong>efficacit\u00e9 thermique<\/strong>\u00a0,\u00a0<strong><em>\u03b7\u00a0<\/em><\/strong><strong><em><sub>th<\/sub><\/em><\/strong>\u00a0, repr\u00e9sente la fraction de\u00a0<strong>chaleur<\/strong>\u00a0,\u00a0<strong>Q\u00a0<\/strong><strong><sub>H<\/sub><\/strong>\u00a0, qui est convertie\u00a0<strong>en travail<\/strong>\u00a0.\u00a0Puisque l&#8217;\u00e9nergie est conserv\u00e9e selon la\u00a0<a href=\"https:\/\/www.thermal-engineering.org\/what-is-first-law-of-thermodynamics-definition\/\"><strong>premi\u00e8re loi de la thermodynamique<\/strong><\/a>\u00a0et que l&#8217;\u00e9nergie ne peut pas \u00eatre convertie pour fonctionner compl\u00e8tement, l&#8217;apport de chaleur, Q\u00a0<sub>H<\/sub>\u00a0, doit \u00eatre \u00e9gal au travail effectu\u00e9, W, plus la chaleur qui doit \u00eatre dissip\u00e9e sous forme de\u00a0<strong>chaleur r\u00e9siduelle Q\u00a0<\/strong><strong><sub>C<\/sub><\/strong>\u00a0dans le environnement.\u00a0Par cons\u00e9quent, nous pouvons r\u00e9\u00e9crire la formule de l&#8217;efficacit\u00e9 thermique comme suit:<\/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-full wp-image-16944 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-2.png\" alt=\"formule d'efficacit\u00e9 thermique - 2\" width=\"352\" height=\"83\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/thermal-efficiency-formula-2.png\" \/><\/a><\/p>\n<p>Par cons\u00e9quent, la chaleur ajout\u00e9e et rejet\u00e9e est donn\u00e9e par:<\/p>\n<p>Q\u00a0<sub>add-1<\/sub>\u00a0= mc\u00a0<sub>v<\/sub>\u00a0(T\u00a0<sub>3<\/sub>\u00a0&#8211; T\u00a0<sub>2<\/sub>\u00a0)<\/p>\n<p>Q\u00a0<sub>add-2<\/sub>\u00a0= mc\u00a0<sub>p<\/sub>\u00a0(T\u00a0<sub>4<\/sub>\u00a0&#8211; T\u00a0<sub>3<\/sub>\u00a0)<\/p>\n<p>Q\u00a0<sub>out<\/sub>\u00a0= mc\u00a0<sub>v<\/sub>\u00a0(T\u00a0<sub>5<\/sub>\u00a0&#8211; T\u00a0<sub>1<\/sub>\u00a0)<\/p>\n<p>Par cons\u00e9quent, l&#8217;efficacit\u00e9 thermique pour un cycle double est:<\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-cycle-thermal-efficiency.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-17669 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-cycle-thermal-efficiency.png\" alt=\"Double cycle - efficacit\u00e9 thermique\" width=\"350\" height=\"75\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dual-cycle-thermal-efficiency.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\"><\/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>Cet article est bas\u00e9 sur la traduction automatique de l&#8217;article original en anglais. Pour plus d&#8217;informations, voir l&#8217;article en anglais. Pouvez vous nous aider Si vous souhaitez corriger la traduction, envoyez-la \u00e0 l&#8217;adresse: translations@nuclear-power.com ou remplissez le formulaire de traduction en ligne. Nous appr\u00e9cions votre aide, nous mettrons \u00e0 jour la traduction le plus rapidement possible. Merci<\/p>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Le Cycle de Sabath\u00e9, ou cycle de pression limit\u00e9, est un cycle thermodynamique qui combine le cycle Otto et le cycle Diesel. Un cycle double comprend cinq processus thermodynamiques. G\u00e9nie thermique Cycle diesel &#8211; moteur diesel Le cycle double\u00a0, ou\u00a0cycle de pression limit\u00e9\u00a0, est un\u00a0cycle thermodynamique\u00a0qui combine le\u00a0cycle Otto\u00a0et le\u00a0cycle Diesel\u00a0.\u00a0Dans le cycle double, la &#8230; <a title=\"Qu&#8217;est-ce qu&#8217;un Cycle de Sabath\u00e9 &#8211; D\u00e9finition\" class=\"read-more\" href=\"https:\/\/www.thermal-engineering.org\/fr\/quest-ce-quun-cycle-double-cycle-de-pression-limite-definition\/\" aria-label=\"En savoir plus sur Qu&#8217;est-ce qu&#8217;un Cycle de Sabath\u00e9 &#8211; D\u00e9finition\">Lire la suite<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[8],"tags":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v15.4 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Qu&#039;est-ce qu&#039;un Cycle de Sabath\u00e9 - Cycle de pression limit\u00e9 - D\u00e9finition<\/title>\n<meta name=\"description\" content=\"Le Cycle de Sabath\u00e9, ou cycle de pression limit\u00e9, est un cycle thermodynamique qui combine le cycle Otto et le cycle Diesel. 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