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Display information for equation id:math.1443.137 on revision:1443

* Page found: Materie in elektrischen und magnetischen Feldern (eq math.1443.137)

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Hash: e1b787816025a6528f1283ccee7be72a

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\begin{align}
& \begin{matrix}
\lim   \\
h->0  \\
\end{matrix}\oint\limits_{\partial V}{{}}d\bar{f}\times \bar{E}=\oint\limits_{\partial V}{{}}df\bar{n}\times \left( {{{\bar{E}}}^{(1)}}-{{{\bar{E}}}^{(2)}} \right)=-\begin{matrix}
\lim   \\
h->0  \\
\end{matrix}\int_{V}^{{}}{{}}{{d}^{3}}r\frac{\partial }{\partial t}\bar{B} \\
& \begin{matrix}
\lim   \\
h->0  \\
\end{matrix}\oint\limits_{\partial V}{{}}d\bar{f}\times H\left( \bar{r},t \right)=\oint\limits_{\partial V}{{}}df\bar{n}\times \left( H{{\left( \bar{r},t \right)}^{(1)}}-H{{\left( \bar{r},t \right)}^{(2)}} \right)=\begin{matrix}
\lim   \\
h->0  \\
\end{matrix}\int_{V}^{{}}{{}}{{d}^{3}}r\left( \bar{j}+\frac{\partial }{\partial t}\bar{D} \right) \\
\end{align}

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limh>0Vdf¯×E¯=Vdfn¯×(E¯(1)E¯(2))=limh>0Vd3rtB¯limh>0Vdf¯×H(r¯,t)=Vdfn¯×(H(r¯,t)(1)H(r¯,t)(2))=limh>0Vd3r(j¯+tD¯)
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