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Display information for equation id:math.1199.334 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.334)

Occurrences on the following pages:

Magnetostatische Feldgleichungen Eq: math.2095.19

Hash: 8c2c63f2e747375e9745391f12b35a60

TeX (original user input):

\nabla \times \bar{B}(\bar{r})=\nabla \left( \nabla \cdot \bar{A}(\bar{r}) \right)-\Delta \bar{A}(\bar{r})={{\mu }_{0}}\bar{j}(\bar{r})+{{\mu }_{0}}{{\varepsilon }_{0}}\frac{\partial }{\partial t}\bar{E}(\bar{r},t)

TeX (checked):

\nabla \times {\bar {B}}({\bar {r}})=\nabla \left(\nabla \cdot {\bar {A}}({\bar {r}})\right)-\Delta {\bar {A}}({\bar {r}})={{\mu }_{0}}{\bar {j}}({\bar {r}})+{{\mu }_{0}}{{\varepsilon }_{0}}{\frac {\partial }{\partial t}}{\bar {E}}({\bar {r}},t)

LaTeXML (experimental; uses MathML) rendering

MathML (15.016 KB / 2.105 KB) :

{\displaystyle{\displaystyle\nabla\times\bar{B}(\bar{r})=\nabla\left(\nabla% \cdot\bar{A}(\bar{r})\right)-\Delta\bar{A}(\bar{r})={{\mu}_{0}}\bar{j}(\bar{r}% )+{{\mu}_{0}}{{\varepsilon}_{0}}\frac{\partial}{\partial t}\bar{E}(\bar{r},t)}}

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    <annotation encoding="application/x-tex" id="p1.1.m1.1c">{\displaystyle{\displaystyle\nabla\times\bar{B}(\bar{r})=\nabla\left(\nabla%
\cdot\bar{A}(\bar{r})\right)-\Delta\bar{A}(\bar{r})={{\mu}_{0}}\bar{j}(\bar{r}%
)+{{\mu}_{0}}{{\varepsilon}_{0}}\frac{\partial}{\partial t}\bar{E}(\bar{r},t)}}</annotation>
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MathML (2.287 KB / 388 B) :

\nabla \times \bar{B} (\bar{r}) = \nabla (\nabla \cdot \bar{A} (\bar{r})) - Δ \bar{A} (\bar{r}) = μ_{0} \bar{j} (\bar{r}) + μ_{0} ε_{0} \frac{\partial}{\partial t} \bar{E} (\bar{r}, t)

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Identifiers

$\bar{B}$

$\bar{r}$

$\bar{A}$

$\bar{r}$

$Δ$

$\bar{A}$

$\bar{r}$

$μ_{0}$

$\bar{j}$

$\bar{r}$

$μ_{0}$

$ε_{0}$

$t$

$\bar{E}$

$\bar{r}$

$t$

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