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@ -361,12 +361,12 @@ Stokes' theorem = |
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for all vectorial field $`\vec{X}`$, |
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$`\displaystyle\iint_{S\,orient.} \;\overrightarrow{rot}\;\overrightarrow{X} \cdot dS = \displaystyle |
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\oint_{\Gamma\,orient.\leftrightarrow S} \overrightarrow{X}\cdot\overrightarrow{dl}`$ |
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\oint_{\Gamma\leftrightarrow S} \overrightarrow{X}\cdot\overrightarrow{dl}`$ |
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$`\displaystyle\oint_{\Gamma\,orient.}\overrightarrow{H} \cdot \overrightarrow{dl}= |
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\underset{S\,orient.}{\iint{\overrightarrow{j}\cdot\overrightarrow{dS}}}`$ |
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\underset{S\leftrightarrow\Gamma}{\iint{\overrightarrow{j}\cdot\overrightarrow{dS}}}`$ |
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$`\displaystyle\left. \dfrac{dQ}{dt}\right|_S =\oint_S \vec{j} \cdot \vec{dS}`$ |
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