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* Page found: Elektrodynamik Schöll (eq math.1199.877)

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\begin{align}
& \Phi \left( \bar{r},t \right)=\frac{1}{\Delta V}\int_{\Delta V}^{{}}{{}}{{d}^{3}}s{{\Phi }_{m}}\left( \bar{r}+\bar{s},t \right)=\frac{1}{4\pi {{\varepsilon }_{0}}}\frac{1}{\Delta V}\int_{\Delta V}^{{}}{{}}{{d}^{3}}s\int_{{{R}^{3}}}^{{}}{{}}{{d}^{3}}r\acute{\ }\frac{{{\rho }_{m}}\left( \bar{r}\acute{\ },t-\frac{\left| \bar{r}+\bar{s}-\bar{r}\acute{\ } \right|}{c} \right)}{\left| \bar{r}+\bar{s}-\bar{r}\acute{\ } \right|} \\
& \bar{r}\acute{\ }\acute{\ }:=\bar{r}\acute{\ }-\bar{s} \\
& \Phi \left( \bar{r},t \right)=\frac{1}{4\pi {{\varepsilon }_{0}}}\frac{1}{\Delta V}\int_{\Delta V}^{{}}{{}}{{d}^{3}}s\int_{{{R}^{3}}}^{{}}{{}}{{d}^{3}}r\acute{\ }\acute{\ }\frac{{{\rho }_{m}}\left( \bar{r}\acute{\ }\acute{\ }+\bar{s},t-\frac{\left| \bar{r}-\bar{r}\acute{\ }\acute{\ } \right|}{c} \right)}{\left| \bar{r}-\bar{r}\acute{\ }\acute{\ } \right|} \\
& =\frac{1}{4\pi {{\varepsilon }_{0}}}\int_{{{R}^{3}}}^{{}}{{}}{{d}^{3}}r\acute{\ }\acute{\ }\frac{1}{\left| \bar{r}-\bar{r}\acute{\ }\acute{\ } \right|}\frac{1}{\Delta V}\int_{\Delta V}^{{}}{{}}{{d}^{3}}s{{\rho }_{m}}\left( \bar{r}\acute{\ }\acute{\ }+\bar{s},t-\frac{\left| \bar{r}-\bar{r}\acute{\ }\acute{\ } \right|}{c} \right) \\
\end{align}

TeX (checked):

{\begin{aligned}&\Phi \left({\bar {r}},t\right)={\frac {1}{\Delta V}}\int _{\Delta V}^{}{}{{d}^{3}}s{{\Phi }_{m}}\left({\bar {r}}+{\bar {s}},t\right)={\frac {1}{4\pi {{\varepsilon }_{0}}}}{\frac {1}{\Delta V}}\int _{\Delta V}^{}{}{{d}^{3}}s\int _{{R}^{3}}^{}{}{{d}^{3}}r{\acute {\ }}{\frac {{{\rho }_{m}}\left({\bar {r}}{\acute {\ }},t-{\frac {\left|{\bar {r}}+{\bar {s}}-{\bar {r}}{\acute {\ }}\right|}{c}}\right)}{\left|{\bar {r}}+{\bar {s}}-{\bar {r}}{\acute {\ }}\right|}}\\&{\bar {r}}{\acute {\ }}{\acute {\ }}:={\bar {r}}{\acute {\ }}-{\bar {s}}\\&\Phi \left({\bar {r}},t\right)={\frac {1}{4\pi {{\varepsilon }_{0}}}}{\frac {1}{\Delta V}}\int _{\Delta V}^{}{}{{d}^{3}}s\int _{{R}^{3}}^{}{}{{d}^{3}}r{\acute {\ }}{\acute {\ }}{\frac {{{\rho }_{m}}\left({\bar {r}}{\acute {\ }}{\acute {\ }}+{\bar {s}},t-{\frac {\left|{\bar {r}}-{\bar {r}}{\acute {\ }}{\acute {\ }}\right|}{c}}\right)}{\left|{\bar {r}}-{\bar {r}}{\acute {\ }}{\acute {\ }}\right|}}\\&={\frac {1}{4\pi {{\varepsilon }_{0}}}}\int _{{R}^{3}}^{}{}{{d}^{3}}r{\acute {\ }}{\acute {\ }}{\frac {1}{\left|{\bar {r}}-{\bar {r}}{\acute {\ }}{\acute {\ }}\right|}}{\frac {1}{\Delta V}}\int _{\Delta V}^{}{}{{d}^{3}}s{{\rho }_{m}}\left({\bar {r}}{\acute {\ }}{\acute {\ }}+{\bar {s}},t-{\frac {\left|{\bar {r}}-{\bar {r}}{\acute {\ }}{\acute {\ }}\right|}{c}}\right)\\\end{aligned}}

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Φ(r¯,t)=1ΔVΔVd3sΦm(r¯+s¯,t)=14πε01ΔVΔVd3sR3d3r´ρm(r¯´,t|r¯+s¯r¯´|c)|r¯+s¯r¯´|r¯´´:=r¯´s¯Φ(r¯,t)=14πε01ΔVΔVd3sR3d3r´´ρm(r¯´´+s¯,t|r¯r¯´´|c)|r¯r¯´´|=14πε0R3d3r´´1|r¯r¯´´|1ΔVΔVd3sρm(r¯´´+s¯,t|r¯r¯´´|c)
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  • ´
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  • r¯
  • ´
  • t
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  • c
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  • ´
  • r¯
  • ´
  • ´
  • r¯
  • ´
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  • Φ
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  • Δ
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  • R
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  • ´
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  • r¯
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  • V
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  • ρm
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