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M3P2
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0654f25b
Commit
0654f25b
authored
Oct 08, 2023
by
Claude Meny
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Update textbook.fr.md
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textbook.fr.md
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12.temporary_ins/20.magnetostatics-vacuum/40.ampere-theorem-applications/10.ampere-integral-method/10.main/textbook.fr.md
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0654f25b
...
@@ -88,7 +88,7 @@ $`\mathcal{\Gamma}_A`$, de *l'orienter* puis de **calculer la circulation** de $
...
@@ -88,7 +88,7 @@ $`\mathcal{\Gamma}_A`$, de *l'orienter* puis de **calculer la circulation** de $
*ÉTAPE 2 :*
**$`\displaystyle\large\mathbf{\oint_{\mathcal{\Gamma}_A}\overrightarrow{B}\cdot\overrightarrow{dl}}`$**
*ÉTAPE 2 :*
**$`\displaystyle\large\mathbf{\oint_{\mathcal{\Gamma}_A}\overrightarrow{B}\cdot\overrightarrow{dl}}`$**
*$`\displaystyle\large = \mu_0\,\sum_{S_A\leftrightarrow\Gamma_A}\,\overline{I}`$*
.
*$`\displaystyle\large = \mu_0\,\sum_{S_A\leftrightarrow\Gamma_A}\,\overline{I}`$*
.
##### Éléments physiques conduisant
à ces choix.
##### Éléments physiques conduisant
au choix du contour
Si le théorème d'Ampère est vrai quelque-soit le contour fermé considéré, aussi complexe soit-il,
Si le théorème d'Ampère est vrai quelque-soit le contour fermé considéré, aussi complexe soit-il,
il ne peut nous aider à calculer le champ magnétique $
`\overrightarrow{B}`
$ dans tout l'espace
il ne peut nous aider à calculer le champ magnétique $
`\overrightarrow{B}`
$ dans tout l'espace
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