Klaus_Hoffmann
- 85
- 1
if we have the Einstein Hilbert action
I= \int_{V} dV (-g)^{1/2}R or I= \int_{V} dV \mathcal L (g_{ab}, \Gamma_{kl}^{i}
then my question is if we can obtain Einstein equations by varying the metric and Christofell symbols independently i mean you get Einstein Field equations by
\frac{\delta I}{\delta g_{ab} =0 \frac{\delta I}{\delta \Gamma_{kl}^{i} =0
i mean , you consider the metric g_{ab} and \Gamma_{kl}^{i} as independent variables for your theory.
I= \int_{V} dV (-g)^{1/2}R or I= \int_{V} dV \mathcal L (g_{ab}, \Gamma_{kl}^{i}
then my question is if we can obtain Einstein equations by varying the metric and Christofell symbols independently i mean you get Einstein Field equations by
\frac{\delta I}{\delta g_{ab} =0 \frac{\delta I}{\delta \Gamma_{kl}^{i} =0
i mean , you consider the metric g_{ab} and \Gamma_{kl}^{i} as independent variables for your theory.