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Display information for equation id:math.1199.1125 on revision:1199
* Page found: Elektrodynamik Schöll (eq math.1199.1125)
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Hash: dd08427fb5ad2ae188d35b8f0fac4781
TeX (original user input):
\begin{align}
& \frac{\omega }{{{c}_{1}}}=\left| {\bar{k}} \right|=\left| \bar{k}\acute{\ } \right|=\frac{\omega \acute{\ }}{{{c}_{1}}} \\
& \left| \bar{k}\acute{\ }\acute{\ } \right|=\frac{\omega \acute{\ }\acute{\ }}{{{c}_{2}}} \\
& {{c}_{i}}=\frac{c}{{{n}_{i}}}=\frac{c}{\sqrt{{{\varepsilon }_{i}}}}\quad i=1,2 \\
& \bar{E}(\bar{r},t)={{{\bar{E}}}_{0}}{{e}^{i\left( \bar{k}\bar{r}-\omega t \right)}} \\
\end{align}
TeX (checked):
{\begin{aligned}&{\frac {\omega }{{c}_{1}}}=\left|{\bar {k}}\right|=\left|{\bar {k}}{\acute {\ }}\right|={\frac {\omega {\acute {\ }}}{{c}_{1}}}\\&\left|{\bar {k}}{\acute {\ }}{\acute {\ }}\right|={\frac {\omega {\acute {\ }}{\acute {\ }}}{{c}_{2}}}\\&{{c}_{i}}={\frac {c}{{n}_{i}}}={\frac {c}{\sqrt {{\varepsilon }_{i}}}}\quad i=1,2\\&{\bar {E}}({\bar {r}},t)={{\bar {E}}_{0}}{{e}^{i\left({\bar {k}}{\bar {r}}-\omega t\right)}}\\\end{aligned}}
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MathML (4.371 KB / 592 B) :
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