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Display information for equation id:math.1199.753 on revision:1199
* Page found: Elektrodynamik Schöll (eq math.1199.753)
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Hash: 3be49d1fe7e7dca0b46908bdfba61555
TeX (original user input):
\begin{align}
& {{\nabla }_{r\acute{\ }}}\cdot \bar{j}(\bar{r}\acute{\ },\tau )=-\frac{\partial }{\partial \tau }\rho (\bar{r}\acute{\ },\tau )=0 \\
& \Rightarrow \dot{\bar{p}}(\tau )=\int_{{}}^{{}}{{}}{{d}^{3}}r\acute{\ }\bar{r}\acute{\ }\dot{\rho }=0 \\
& \Rightarrow {{A}^{(1)}}=\frac{{{\mu }_{0}}}{4\pi r}\dot{\bar{p}}(\tau )\equiv 0 \\
\end{align}
TeX (checked):
{\begin{aligned}&{{\nabla }_{r{\acute {\ }}}}\cdot {\bar {j}}({\bar {r}}{\acute {\ }},\tau )=-{\frac {\partial }{\partial \tau }}\rho ({\bar {r}}{\acute {\ }},\tau )=0\\&\Rightarrow {\dot {\bar {p}}}(\tau )=\int _{}^{}{}{{d}^{3}}r{\acute {\ }}{\bar {r}}{\acute {\ }}{\dot {\rho }}=0\\&\Rightarrow {{A}^{(1)}}={\frac {{\mu }_{0}}{4\pi r}}{\dot {\bar {p}}}(\tau )\equiv 0\\\end{aligned}}
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