Maxwell-Gleichungen: Unterschied zwischen den Versionen

Aktuelle Version vom 12. September 2010, 17:37 Uhr

F^{α} {^{β}}_{, β} = μ_{0} j^{α}

F_{⟨ α β γ ⟩} = 0

{F^{μ}}^{ν} = A^{[μ, ν]}

E = \frac{1}{c} E_{r e a l}

A^{μ} = (ϕ, \vec{A})

j^{μ} = (c ρ, \vec{j})

{F^{μ}}^{ν} = (\begin{matrix} - E_{1} & - E_{2} & - E_{3} \\ - B_{3} & B_{2} \\ - B_{1} \end{matrix})

@@ Zeile 1: / Zeile 1: @@
-<math>{{\partial }_{\alpha }}{{F}^{\alpha }}^{\beta }={{j}^{\beta }}</math>
+:<math>{{F}^{\alpha }}{{^{\beta }}_{,\beta }}={{\mu }_{0}}{{j}^{\alpha }}</math>
-<math>{{\partial }_{<}}_{\alpha }{{F}_{\beta \gamma >}}=0</math>
+:<math>{{F}_{\left\langle \alpha \beta \gamma  \right\rangle }}=0</math>
+:<math>{{F}^{\mu }}^{\nu }={{A}^{\left[ \mu ,\nu  \right]}}</math>
+:<math>E=\frac{1}{c}{{E}_{real}}</math>
+:<math>{{A}^{\mu }}=\left( \phi ,\vec{A} \right)</math>
+:<math>{{j}^{\mu }}=\left( c\rho ,\vec{j} \right)</math>
+:<math>{{F}^{\mu }}^{\nu }=\left( \begin{matrix}
+   {} & -{{E}_{1}} & -{{E}_{2}} & -{{E}_{3}}  \\
+   {} & {} & -{{B}_{3}} & {{B}_{2}}  \\
+   {} & {} & {} & -{{B}_{1}}  \\
+   {} & {} & {} & {}  \\
+\end{matrix} \right)</math>
+[[Kategorie:Tensor_2._Stufe]]