{"id":82587,"date":"2024-01-14T13:21:51","date_gmt":"2024-01-14T13:21:51","guid":{"rendered":"https:\/\/www.electricity-magnetism.org\/theoreme-de-thevenin-analyse-des-circuits\/"},"modified":"2024-01-23T13:14:36","modified_gmt":"2024-01-23T13:14:36","slug":"theoreme-de-thevenin-analyse-des-circuits","status":"publish","type":"post","link":"https:\/\/www.electricity-magnetism.org\/fr\/theoreme-de-thevenin-analyse-des-circuits\/","title":{"rendered":"Th\u00e9or\u00e8me de Th\u00e9venin | Analyse des circuits"},"content":{"rendered":"<h2>Le Th\u00e9or\u00e8me de Th\u00e9venin<\/h2>\n<p>Le Th\u00e9or\u00e8me de Th\u00e9venin est une technique fondamentale en g\u00e9nie \u00e9lectrique, utilis\u00e9e pour simplifier les circuits lin\u00e9aires complexes, particuli\u00e8rement lors de l&rsquo;analyse ou de la conception de circuits avec de multiples composants. Ce th\u00e9or\u00e8me \u00e9nonce qu&rsquo;un circuit bipolaire lin\u00e9aire et invariant dans le temps peut \u00eatre remplac\u00e9 par un circuit \u00e9quivalent compos\u00e9 d&rsquo;une unique source de tension (tension de Th\u00e9venin, V<sub>th<\/sub>) en s\u00e9rie avec une unique r\u00e9sistance (r\u00e9sistance de Th\u00e9venin, R<sub>th<\/sub>), \u00e0 condition que le comportement de la tension et du courant de sortie aux bornes reste identique.<\/p>\n<h2>Application du Th\u00e9or\u00e8me de Th\u00e9venin<\/h2>\n<p>Pour appliquer le Th\u00e9or\u00e8me de Th\u00e9venin, suivez ces \u00e9tapes :<\/p>\n<p>Retirer la r\u00e9sistance de charge (R<sub>L<\/sub>) du circuit, en laissant les deux bornes o\u00f9 la r\u00e9sistance de charge \u00e9tait connect\u00e9e.<br \/>\nCalculer la tension \u00e0 vide aux bornes, qui est la tension de Th\u00e9venin (V<sub>th<\/sub>). Cette tension peut \u00eatre trouv\u00e9e en utilisant diverses techniques d&rsquo;analyse de circuit, telles que la Loi d&rsquo;Ohm, les Lois de Kirchhoff, ou l&rsquo;analyse des tensions de n\u0153ud.<br \/>\nRemplacer toutes les sources de tension par des courts-circuits et toutes les sources de courant par des circuits ouverts. Calculer la r\u00e9sistance \u00e9quivalente vue depuis les bornes, qui est la r\u00e9sistance de Th\u00e9venin (R<sub>th<\/sub>). Cette r\u00e9sistance peut \u00eatre trouv\u00e9e en utilisant des combinaisons de r\u00e9sistances en s\u00e9rie et en parall\u00e8le ou en appliquant d&rsquo;autres techniques, telles que la transformation delta-en-Y.<br \/>\nRemplacer le circuit original par le circuit \u00e9quivalent de Th\u00e9venin, compos\u00e9 de la tension de Th\u00e9venin (V<sub>th<\/sub>) en s\u00e9rie avec la r\u00e9sistance de Th\u00e9venin (R<sub>th<\/sub>).<br \/>\nReconnecter la r\u00e9sistance de charge (R<sub>L<\/sub>) aux bornes du circuit \u00e9quivalent de Th\u00e9venin.<\/p>\n<h2>Avantages du Th\u00e9or\u00e8me de Th\u00e9venin<\/h2>\n<p>Avec le circuit \u00e9quivalent de Th\u00e9venin simplifi\u00e9, vous pouvez maintenant analyser le circuit plus facilement, par exemple en d\u00e9terminant le courant traversant la r\u00e9sistance de charge ou en trouvant le transfert de puissance maximal. Gardez \u00e0 l&rsquo;esprit que le Th\u00e9or\u00e8me de Th\u00e9venin ne peut \u00eatre appliqu\u00e9 qu&rsquo;aux circuits lin\u00e9aires et invariants dans le temps ; il ne s&rsquo;applique pas aux circuits avec des composants non lin\u00e9aires ou variant dans le temps.<\/p>\n<h2>Autres Th\u00e9or\u00e8mes de Circuit<\/h2>\n<p>Les th\u00e9or\u00e8mes de circuit sont des outils essentiels pour analyser et simplifier des circuits \u00e9lectriques complexes. Ils aident les ing\u00e9nieurs et les techniciens \u00e0 trouver des circuits \u00e9quivalents, \u00e0 r\u00e9soudre des quantit\u00e9s inconnues et \u00e0 optimiser les performances des circuits. Parmi les th\u00e9or\u00e8mes de circuit les plus importants, on trouve :<\/p>\n<p>Loi d&rsquo;Ohm<br \/>\nLois de Kirchhoff<br \/>\nTh\u00e9or\u00e8me de Th\u00e9venin<br \/>\nTh\u00e9or\u00e8me de Norton<br \/>\nTh\u00e9or\u00e8me de Superposition<br \/>\nTh\u00e9or\u00e8me du Transfert de Puissance Maximale<br \/>\nTransformations Delta-en-Y (\u0394-Y) et Y-en-Delta (Y-\u0394)<\/p>\n<h2>Article Suivant<\/h2>\n<p>Dans le prochain article, nous explorerons plus en d\u00e9tail le Th\u00e9or\u00e8me de Norton, un autre outil puissant pour l&rsquo;analyse de circuits \u00e9lectriques.<\/p>\n<p><img decoding=\"async\" src=\"https:\/\/www.electricity-magnetism.org\/wp-content\/uploads\/2022\/01\/logo.png\" alt=\"Thevenin's Theorem\" \/><\/p>\n<div style=\"text-align: center; font-size: 20px;\">\n    <a href=\"https:\/\/www.electricity-magnetism.org\/thevenins-theorem\/\">Original Article<\/a>\n<\/div>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Le th\u00e9or\u00e8me de Th\u00e9venin est une technique fondamentale utilis\u00e9e en g\u00e9nie \u00e9lectrique pour simplifier des circuits lin\u00e9aires complexes, en particulier lors de l&rsquo;analyse ou de la conception de circuits \u00e0 composants multiples.<\/p>\n","protected":false},"author":1,"featured_media":1576,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_generate-full-width-content":"","footnotes":""},"categories":[10],"tags":[],"class_list":["post-82587","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-non-classifiee","generate-columns","tablet-grid-50","mobile-grid-100","grid-parent","grid-50"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v17.9 - 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