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Commit 31cac192 authored by Claude Meny's avatar Claude Meny
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Update textbook.en.md

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    10.brainstorming-innovative-courses/intercambio-curso-electromagnetismo/textbook.en.md
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    ...@@ -634,7 +634,7 @@ $`\overrightarrow{rot}\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}`$ ...@@ -634,7 +634,7 @@ $`\overrightarrow{rot}\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}`$
    Electromagnétisme dans le vide : Electromagnétisme dans le vide :
    $`\overrightarrow{rot}\,\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}\,+ \, \epsilon_0\mu_0 \cdot \dfrac{\partial \overrightarrow{E}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \, \dfrac{1}{c^2} \cdot \dfrac{\partial \overrightarrow{E}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \mu_0 \cdot \overrightarrow{j_D} = \mu_0 \cdot (\overrightarrow{j}+\overrightarrow{j_D})`$ $`\overrightarrow{rot}\,\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}\,+ \, \epsilon_0\mu_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \, \dfrac{1}{c^2} \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \mu_0 \cdot \overrightarrow{j_D} = \mu_0 \cdot (\overrightarrow{j}+\overrightarrow{j_D})`$
    avec $`\overrightarrow{j_D}`$ courant de déplacement : $`\overrightarrow{j_D}=\epsilon_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$ avec $`\overrightarrow{j_D}`$ courant de déplacement : $`\overrightarrow{j_D}=\epsilon_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$
    ...@@ -678,11 +678,11 @@ $`\epsilon_0 \cdot \mu_0 \cdot c^2 = 1`$ ...@@ -678,11 +678,11 @@ $`\epsilon_0 \cdot \mu_0 \cdot c^2 = 1`$
    $`div\overrightarrow{E}=\dfrac{\rho}{\epsilon_0}`$ $`div\overrightarrow{E}=\dfrac{\rho}{\epsilon_0}`$
    $`rot\overrightarrow{E}=-\dfrac{\partial \overrightarrow{B}}{\partial t}`$ $`\overrightarrow{rot}\overrightarrow{E}=-\dfrac{\partial \overrightarrow{B}}{\partial t}`$
    $`div\overrightarrow{B}=0`$ $`div\overrightarrow{B}=0`$
    $`rot\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}\,+ \, \epsilon_0\mu_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \, \dfrac{1}{c^2} \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$ $`\overrightarrow{rot}\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}\,+ \, \epsilon_0\mu_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$$`=\mu_0 \cdot \overrightarrow{j}\,+ \, \dfrac{1}{c^2} \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$
    #### Ecuaciones de Maxwell en forma integral / Equations de maxwell intégrales / ... #### Ecuaciones de Maxwell en forma integral / Equations de maxwell intégrales / ...
    ......
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