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Claude Meny 6 years ago
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      10.brainstorming-innovative-courses/intercambio-curso-electromagnetismo/textbook.en.md

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10.brainstorming-innovative-courses/intercambio-curso-electromagnetismo/textbook.en.md

@ -634,13 +634,13 @@ $`\overrightarrow{rot}\overrightarrow{B}=\mu_0 \cdot \overrightarrow{j}`$
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 (j+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 : $`\overrightarrow{j_D}=\epsilon_0 \cdot \dfrac{\partial \overrightarrow{E}}{\partial t}`$
Con corriente de desplazamiento
$`\overrightarrow{rot}\overrightarrow{E}=-\dfrac{\partial \overrightarrow{B}}{\partial t}`$
$`\overrightarrow{rot}\,\overrightarrow{E}=-\dfrac{\partial \overrightarrow{B}}{\partial t}`$
$`div\overrightarrow{E}=\dfrac{\rho}{\epsilon_0}`$

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