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$div\vec{E} = \frac{\rho}{\epsilon_{0}}$
Maxwell-Gauss en statique
$div\vec{B} = 0$
Maxwell-flux en statique
$\vec{rot}\vec{E} = -\frac{\partial\vec{B}}{\partial t}$
Maxwell-Faraday en statique
$\vec{rot}\vec{B} = \mu_{0}\vec{j} + \mu_{0}\epsilon_{0}\frac{\partial\vec{E}}{\partial t}$
Maxwell-Ampère en statique
