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Display information for equation id:math.1199.414 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.414)

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Hash: 0f83e567e528535eeec30e335a524bb9

TeX (original user input):

\begin{align}
& {{\nabla }_{r}}\times \bar{E}={{a}_{1}}\dot{\bar{E}}+{{b}_{1}}\dot{\bar{B}} \\
& \nabla \times \bar{B}-{{\mu }_{0}}\bar{j}={{a}_{2}}\dot{\bar{E}}+{{b}_{2}}\dot{\bar{B}} \\
& {{\varepsilon }_{0}}{{\nabla }_{r}}\cdot \bar{E}-\rho =0 \\
& {{\nabla }_{r}}\cdot \bar{B}=0 \\
\end{align}

TeX (checked):

{\begin{aligned}&{{\nabla }_{r}}\times {\bar {E}}={{a}_{1}}{\dot {\bar {E}}}+{{b}_{1}}{\dot {\bar {B}}}\\&\nabla \times {\bar {B}}-{{\mu }_{0}}{\bar {j}}={{a}_{2}}{\dot {\bar {E}}}+{{b}_{2}}{\dot {\bar {B}}}\\&{{\varepsilon }_{0}}{{\nabla }_{r}}\cdot {\bar {E}}-\rho =0\\&{{\nabla }_{r}}\cdot {\bar {B}}=0\\\end{aligned}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.843 KB / 430 B) :

r×E¯=a1E¯˙+b1B¯˙×B¯μ0j¯=a2E¯˙+b2B¯˙ε0rE¯ρ=0rB¯=0
<math class="mwe-math-element" xmlns="http://www.w3.org/1998/Math/MathML"><mrow data-mjx-texclass="ORD"><mstyle displaystyle="true" scriptlevel="0"><mrow data-mjx-texclass="ORD"><mtable columnalign="right left right left right left right left right left right left" columnspacing="0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0em" displaystyle="true" rowspacing="3pt"><mtr><mtd></mtd><mtd><msub><mi mathvariant="normal">&#x2207;</mi><mrow data-mjx-texclass="ORD"><mi>r</mi></mrow></msub><mo>&#x00D7;</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>E</mi><mo>¯</mo></mover></mrow></mrow><mo>=</mo><msub><mi>a</mi><mrow data-mjx-texclass="ORD"><mn>1</mn></mrow></msub><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>E</mi><mo>¯</mo></mover></mrow></mrow><mo>˙</mo></mover></mrow></mrow><mo>+</mo><msub><mi>b</mi><mrow data-mjx-texclass="ORD"><mn>1</mn></mrow></msub><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>B</mi><mo>¯</mo></mover></mrow></mrow><mo>˙</mo></mover></mrow></mrow></mtd></mtr><mtr><mtd></mtd><mtd><mi mathvariant="normal">&#x2207;</mi><mo>&#x00D7;</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>B</mi><mo>¯</mo></mover></mrow></mrow><mo>&#x2212;</mo><msub><mi>&#x03BC;</mi><mrow data-mjx-texclass="ORD"><mn>0</mn></mrow></msub><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>j</mi><mo>¯</mo></mover></mrow></mrow><mo>=</mo><msub><mi>a</mi><mrow data-mjx-texclass="ORD"><mn>2</mn></mrow></msub><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>E</mi><mo>¯</mo></mover></mrow></mrow><mo>˙</mo></mover></mrow></mrow><mo>+</mo><msub><mi>b</mi><mrow data-mjx-texclass="ORD"><mn>2</mn></mrow></msub><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>B</mi><mo>¯</mo></mover></mrow></mrow><mo>˙</mo></mover></mrow></mrow></mtd></mtr><mtr><mtd></mtd><mtd><msub><mi>&#x03B5;</mi><mrow data-mjx-texclass="ORD"><mn>0</mn></mrow></msub><msub><mi mathvariant="normal">&#x2207;</mi><mrow data-mjx-texclass="ORD"><mi>r</mi></mrow></msub><mo>&#x22C5;</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>E</mi><mo>¯</mo></mover></mrow></mrow><mo>&#x2212;</mo><mi>&#x03C1;</mi><mo>=</mo><mn>0</mn></mtd></mtr><mtr><mtd></mtd><mtd><msub><mi mathvariant="normal">&#x2207;</mi><mrow data-mjx-texclass="ORD"><mi>r</mi></mrow></msub><mo>&#x22C5;</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>B</mi><mo>¯</mo></mover></mrow></mrow><mo>=</mo><mn>0</mn></mtd></mtr><mtr><mtd></mtd></mtr></mtable></mrow></mstyle></mrow></math>

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Calculated based on the variables occurring on the entire Elektrodynamik Schöll page

Identifiers

  • r
  • E¯
  • a1
  • E¯˙
  • b1
  • B¯˙
  • B¯
  • μ0
  • j¯
  • a2
  • E¯˙
  • b2
  • B¯˙
  • ε0
  • r
  • E¯
  • ρ
  • r
  • B¯

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