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Display information for equation id:math.2171.41 on revision:2171

* Page found: Transformationsverhalten der Ströme und Felder (eq math.2171.41)

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Hash: a6ed87de17a3025a8d48ced5b306e188

TeX (original user input): 

\begin{align}
& \nabla \cdot \bar{B}={{\partial }_{1}}{{B}^{1}}+{{\partial }_{2}}{{B}^{2}}+{{\partial }_{3}}{{B}^{3}}=0 \\
& \Rightarrow {{\partial }_{1}}{{F}^{32}}+{{\partial }_{2}}{{F}^{13}}+{{\partial }_{3}}{{F}^{21}}=0 \\
&  \\
\end{align}

TeX (checked): 

{\begin{aligned}&\nabla \cdot {\bar {B}}={{\partial }_{1}}{{B}^{1}}+{{\partial }_{2}}{{B}^{2}}+{{\partial }_{3}}{{B}^{3}}=0\\&\Rightarrow {{\partial }_{1}}{{F}^{32}}+{{\partial }_{2}}{{F}^{13}}+{{\partial }_{3}}{{F}^{21}}=0\\&\\\end{aligned}}

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MathML (17.521 KB / 2.069 KB) :

∇ ⋅ B ¯ = ∂ 1 ⁡ B 1 + ∂ 2 ⁡ B 2 + ∂ 3 ⁡ B 3 = 0 ⇒ ∂ 1 ⁡ F 32 + ∂ 2 ⁡ F 13 + ∂ 3 ⁡ F 21 = 0 missing-subexpression ⋅ ∇ ¯ 𝐵 subscript 1 superscript 𝐵 1 subscript 2 superscript 𝐵 2 subscript 3 superscript 𝐵 3 0 missing-subexpression ⇒ absent subscript 1 superscript 𝐹 32 subscript 2 superscript 𝐹 13 subscript 3 superscript 𝐹 21 0 missing-subexpression missing-subexpression {\displaystyle{\displaystyle\begin{aligned} &\displaystyle\nabla\cdot\bar{B}={% {\partial}_{1}}{{B}^{1}}+{{\partial}_{2}}{{B}^{2}}+{{\partial}_{3}}{{B}^{3}}=0% \\ &\displaystyle\Rightarrow{{\partial}_{1}}{{F}^{32}}+{{\partial}_{2}}{{F}^{13}}% +{{\partial}_{3}}{{F}^{21}}=0\\ &\\ \end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.775 KB / 385 B) :

∇⋅B¯=∂1B1+∂2B2+∂3B3=0⇒∂1F32+∂2F13+∂3F21=0

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  • B
  • B
  • B
  • F
  • F
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