Update cheatsheet.fr.md

12.temporary_ins/20.magnetostatics-vacuum/30.ampere-therorem-demonstration/20.overview/cheatsheet.fr.md

@@ -549,16 +549,26 @@ sera ainsi un *courant local*.
   lequel la norme $`\Vert\overrightarrow{X}\Vert`$ calculée sur tous les dC possibles prend sa valeur maximale :   
   <br> 
   **$`\mathbf{\Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert=\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}`$**
-  **$`\mathbf{=\dfrac{d\mathcal{C}_{\overrightarrow{X}}{dS}}`$**
+  **$`\mathbf{=\dfrac{d\mathcal{C}_{\overrightarrow{X}}}{dS}}`$**
 
   $`\begin{align}
-  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert&=\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
-  =\dfrac{d\mathcal{C}_{\overrightarrow{X}}{dS}
+  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert & =\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
+  & =\dfrac{d\mathcal{C}_{\overrightarrow{X}}}{dS}
+\end{align}`$
+
+  $`\begin{align}
+  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert & =\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
+  & =\dfrac{d\mathcal{C}_{\overrightarrow{X}}}{dS} \\
+\end{align}`$
+
+  $`\begin{align}
+  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert &=\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
+  &=\dfrac{d\mathcal{C}_{\overrightarrow{X}}}{dS}
 \end{align}`$
 
   **$`\begin{align}
-  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert&=\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
-  =\dfrac{d\mathcal{C}_{\overrightarrow{X}}{dS}
+  \Vert\overrightarrow{rot}\,\overrightarrow{X}\Vert &=\left(\displaystyle \lim_{C_{\circlearrowleft}\,\longrightarrow 0 \\ C_{\circlearrowleft} \leftrightarrow S_{\circlearrowleft}} \dfrac{\displaystyle\oint_C \overrightarrow{X}\cdot\overrightarrow{dC}}{\displaystyle\iint_S dS}\right)_{MAX}}\\
+  &=\dfrac{d\mathcal{C}_{\overrightarrow{X}}}{dS}
 \end{align}`$**