Kovariante Ableitung
Aus PhysikWiki
\begin{align} T_{{\color{Orange}rs...}; \color{Red}l}^{\color{Blue}ik...} = T_{{\color{Orange}rs...}, \color{Red}l}^{\color{Blue} ik...}& + \Gamma _{ m\color{Red}l}^{\color{Blue}i}T_{\color{Orange}rs...}^{m\color{Blue}k...}\quad&& + \Gamma _{m\color{Red}l}^{\color{Blue}i}T_{\color{Orange}rs...}^{{\color{Blue}r}m\color{Blue}...}... &\quad& {\color{Blue}\text{f }\!\!\ddot{\mathrm{u}}\!\!\text{ r jeden oberen Index}} \\ & + \Gamma _{\color{Orange}r\color{Red}l}^{m}T_{m\color{Orange}s...}^{ \color{Blue}ik...}\quad&& + \Gamma _{\color{Orange}r\color{Red}l}^{m}T_{{\color{Orange}r}m\color{Orange}...}^{ \color{Blue}ik...}...&& \color{Orange}{\text{f }\!\!\ddot{\mathrm{u}}\!\!\text{ r jeden unteren Index}} \\ \end{align}
Eigenschaften
- erhält Tensoreingeschaft <-> Unterschied zur gewöhnlichen Ableitung
