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Display information for equation id:math.1199.155 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.155)

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Hash: 30356b668a2c8eaf7ac19464bb50fe63

TeX (original user input):

\begin{align}
& {{Q}_{2}}=\frac{1}{2{{r}^{2}}}{{Q}_{kl}} \\
& \int_{-\infty }^{\infty }{{}}{{d}^{3}}r\acute{\ }\rho (\bar{r}\acute{\ })\left( 3{{x}_{k}}\acute{\ }{{x}_{l}}\acute{\ }-\bar{r}{{\acute{\ }}^{2}}{{\delta }_{kl}} \right)={{Q}_{kl}} \\
\end{align}

TeX (checked):

{\begin{aligned}&{{Q}_{2}}={\frac {1}{2{{r}^{2}}}}{{Q}_{kl}}\\&\int _{-\infty }^{\infty }{}{{d}^{3}}r{\acute {\ }}\rho ({\bar {r}}{\acute {\ }})\left(3{{x}_{k}}{\acute {\ }}{{x}_{l}}{\acute {\ }}-{\bar {r}}{{\acute {\ }}^{2}}{{\delta }_{kl}}\right)={{Q}_{kl}}\\\end{aligned}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.902 KB / 557 B) :

Q2=12r2Qkld3r´ρ(r¯´)(3xk´xl´r¯´2δkl)=Qkl
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Identifiers

  • Q2
  • r
  • Qkl
  • r
  • ´
  • ρ
  • r¯
  • ´
  • xk
  • ´
  • xl
  • ´
  • r¯
  • ´
  • δkl
  • Qkl

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