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Display information for equation id:math.2147.22 on revision:2147

* Page found: Maxwell- Gleichungen in Materie (eq math.2147.22)

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TeX (original user input): 

4)\nabla \times H\left( \bar{r},t \right)-\frac{1}{c}\frac{\partial }{\partial t}\bar{D}=\frac{4\pi }{c}\bar{j}

TeX (checked): 

4)\nabla \times H\left({\bar {r}},t\right)-{\frac {1}{c}}{\frac {\partial }{\partial t}}{\bar {D}}={\frac {4\pi }{c}}{\bar {j}}

LaTeXML (experimental; uses MathML) rendering

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4 ) ∇ × H ( r ¯ , t ) - 1 c ∂ ∂ ⁡ t D ¯ = 4 ⁢ π c j ¯ fragments 4 ) ∇ H ( ¯ 𝑟 , t ) 1 𝑐 𝑡 ¯ 𝐷 4 𝜋 𝑐 ¯ 𝑗 {\displaystyle{\displaystyle 4)\nabla\times H\left(\bar{r},t\right)-\frac{1}{c% }\frac{\partial}{\partial t}\bar{D}=\frac{4\pi}{c}\bar{j}}} 
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MathML (2.294 KB / 587 B) :

4 ) ∇ × H ( r ¯ , t ) − 1 c ∂ ∂ t D ¯ = 4 π c j ¯ {\displaystyle 4)\nabla \times H\left({\bar {r}},t\right)-{\frac {1}{c}}{\frac {\partial }{\partial t}}{\bar {D}}={\frac {4\pi }{c}}{\bar {j}}} 
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SVG (9.775 KB / 4.035 KB) :

{\displaystyle 4)\nabla \times H\left({\bar {r}},t\right)-{\frac {1}{c}}{\frac {\partial }{\partial t}}{\bar {D}}={\frac {4\pi }{c}}{\bar {j}}}

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