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Display information for equation id:math.1199.378 on revision:1199
* Page found: Elektrodynamik Schöll (eq math.1199.378)
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TeX (original user input):
\begin{align}
& \bar{m}=\frac{1}{2}\oint\limits_{L}{{}}{{d}^{3}}r\acute{\ }\left( \bar{r}\acute{\ }\times \bar{j}(\bar{r}\acute{\ }) \right)=\frac{1}{2}\sum\limits_{i}{{}}{{q}_{i}}\int_{{}}^{{}}{{}}{{d}^{3}}r\acute{\ }\bar{r}\acute{\ }\times {{{\bar{v}}}_{i}}\delta \left( \bar{r}\acute{\ }-{{{\bar{r}}}_{i}} \right)=\frac{1}{2}\sum\limits_{i}{{}}{{q}_{i}}{{{\bar{r}}}_{i}}\times {{{\bar{v}}}_{i}}=\frac{1}{2}\sum\limits_{i}{{}}\frac{{{q}_{i}}}{{{m}_{i}}}{{m}_{i}}{{{\bar{r}}}_{i}}\times {{{\bar{v}}}_{i}} \\
& \frac{{{q}_{i}}}{{{m}_{i}}}=\frac{q}{m} \\
& \Rightarrow \bar{m}=\frac{q}{2m}\bar{L} \\
\end{align}
TeX (checked):
{\begin{aligned}&{\bar {m}}={\frac {1}{2}}\oint \limits _{L}{}{{d}^{3}}r{\acute {\ }}\left({\bar {r}}{\acute {\ }}\times {\bar {j}}({\bar {r}}{\acute {\ }})\right)={\frac {1}{2}}\sum \limits _{i}{}{{q}_{i}}\int _{}^{}{}{{d}^{3}}r{\acute {\ }}{\bar {r}}{\acute {\ }}\times {{\bar {v}}_{i}}\delta \left({\bar {r}}{\acute {\ }}-{{\bar {r}}_{i}}\right)={\frac {1}{2}}\sum \limits _{i}{}{{q}_{i}}{{\bar {r}}_{i}}\times {{\bar {v}}_{i}}={\frac {1}{2}}\sum \limits _{i}{}{\frac {{q}_{i}}{{m}_{i}}}{{m}_{i}}{{\bar {r}}_{i}}\times {{\bar {v}}_{i}}\\&{\frac {{q}_{i}}{{m}_{i}}}={\frac {q}{m}}\\&\Rightarrow {\bar {m}}={\frac {q}{2m}}{\bar {L}}\\\end{aligned}}
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