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Display information for equation id:math.1199.520 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.520)

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Hash: ffdee47c91cd46ec69b9e03434f62edd

TeX (original user input): 

\oint\limits_{\partial F}{d\bar{s}}\bar{A}\left( \bar{r},t \right)=\int_{F}^{{}}{d\bar{f}\bar{B}\left( \bar{r},t \right)=\Phi \left( \bar{r},t \right)}

TeX (checked): 

\oint \limits _{\partial F}{d{\bar {s}}}{\bar {A}}\left({\bar {r}},t\right)=\int _{F}^{}{d{\bar {f}}{\bar {B}}\left({\bar {r}},t\right)=\Phi \left({\bar {r}},t\right)}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (10.49 KB / 1.632 KB) :

∮ ∂ ⁡ F 𝑑 s ¯ ⁢ A ¯ ⁢ ( r ¯ , t ) = ∫ F 𝑑 f ¯ ⁢ B ¯ ⁢ ( r ¯ , t ) = Φ ⁢ ( r ¯ , t ) subscript contour-integral 𝐹 differential-d ¯ 𝑠 ¯ 𝐴 ¯ 𝑟 𝑡 subscript 𝐹 differential-d ¯ 𝑓 ¯ 𝐵 ¯ 𝑟 𝑡 Φ ¯ 𝑟 𝑡 {\displaystyle{\displaystyle\oint\limits_{\partial F}{d\bar{s}}\bar{A}\left(% \bar{r},t\right)=\int_{F}{d\bar{f}\bar{B}\left(\bar{r},t\right)=\Phi\left(\bar% {r},t\right)}}} 
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MathML (experimentell; keine Bilder) rendering

MathML (1.805 KB / 353 B) :

∮∂Fds¯A¯(r¯,t)=∫Fdf¯B¯(r¯,t)=Φ(r¯,t)
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Calculated based on the variables occurring on the entire Elektrodynamik Schöll page

Identifiers

  • F
  • d
  • s¯
  • A¯
  • r¯
  • t
  • F
  • f¯
  • B¯
  • r¯
  • t
  • Φ
  • r¯
  • t

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