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Commit 01d04b09 authored by Claude Meny's avatar Claude Meny
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Update textbook.fr.md

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    12.temporary_ins/20.magnetostatics-vacuum/40.ampere-theorem-applications/05.ampere-symetries-invariances/10.main/textbook.fr.md
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    ...@@ -194,11 +194,11 @@ Si de plus la distribution de courants $`\overrightarrow{j}`$ est invariante par ...@@ -194,11 +194,11 @@ Si de plus la distribution de courants $`\overrightarrow{j}`$ est invariante par
    \end{array}\right\}}`$ \end{array}\right\}}`$
    $`\mathbf{\Longrightarrow \overrightarrow{j} = \overrightarrow{j} (\beta)\Longrightarrow \overrightarrow{B}=\overrightarrow{B}\,(\beta)}`$** $`\mathbf{\Longrightarrow \overrightarrow{j} = \overrightarrow{j} (\beta)\Longrightarrow \overrightarrow{B}=\overrightarrow{B}\,(\beta)}`$**
    $`\begin{align}\left. $`\require{cancel}\begin{align}\left.
    \begin{align} \begin{array}
    &\overrightarrow{j}\,(\xcancel{\alpha},\beta, \gamma) =\overrightarrow{j}\,(\beta,\gamma) \\ &\overrightarrow{j}\,(\xcancel{\alpha},\beta, \gamma) =\overrightarrow{j}\,(\beta,\gamma) \\
    &\overrightarrow{j}\,(\alpha,\beta, \xcancel{\gamma}) =\overrightarrow{j}\,(\alpha,\beta) &\overrightarrow{j}\,(\alpha,\beta, \xcancel{\gamma}) =\overrightarrow{j}\,(\alpha,\beta)
    \end{align}\right\}&\Longrightarrow \overrightarrow{j} = \overrightarrow{j} (\beta)\\ \end{array}\right\}&\Longrightarrow \overrightarrow{j} = \overrightarrow{j} (\beta)\\
    &\Longrightarrow \overrightarrow{B}=\overrightarrow{B}\,(\beta) &\Longrightarrow \overrightarrow{B}=\overrightarrow{B}\,(\beta)
    \end{align}`$ \end{align}`$
    ......
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