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Display information for equation id:math.1199.1004 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.1004)

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Hash: deaf72bb98d099f13d42fc805a254f09

TeX (original user input): 

4)\nabla \times H\left( \bar{r},t \right)=\bar{j}+\frac{\partial }{\partial t}\bar{D}\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \bar{n}\times \delta H\left( \bar{r},t \right)=\bar{g}

TeX (checked): 

4)\nabla \times H\left({\bar {r}},t\right)={\bar {j}}+{\frac {\partial }{\partial t}}{\bar {D}}\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad {\bar {n}}\times \delta H\left({\bar {r}},t\right)={\bar {g}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (7.095 KB / 1.324 KB) :

4 ) ∇ × H ( r ¯ , t ) = j ¯ + ∂ ∂ ⁡ t D ¯            n ¯ × δ H ( r ¯ , t ) = g ¯ fragments 4 ) ∇ H ( ¯ 𝑟 , t ) ¯ 𝑗 𝑡 ¯ 𝐷 italic-           ¯ 𝑛 δ H ( ¯ 𝑟 , t ) ¯ 𝑔 {\displaystyle{\displaystyle 4)\nabla\times H\left(\bar{r},t\right)=\bar{j}+% \frac{\partial}{\partial t}\bar{D}\quad\quad\quad\quad\quad\quad\quad\quad% \quad\quad\bar{n}\times\delta H\left(\bar{r},t\right)=\bar{g}}} 
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4)∇×H(r¯,t)=j¯+∂∂tD¯n¯×δH(r¯,t)=g¯
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Calculated based on the variables occurring on the entire Elektrodynamik Schöll page

Identifiers

  • H
  • r¯
  • t
  • j¯
  • t
  • D¯
  • n¯
  • δ
  • H
  • r¯
  • t
  • g¯

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