- #1
Einj
- 470
- 59
Hello everyone. I'm reading Weinberg's 'Gravitation and Cosmology' and I'm having some problems understanding the definition of a 'form-invariat function'. He says:
\begin{equation}
g^\prime_{\mu\nu}(x^\prime)=g_{\mu\nu}(x)
\end{equation}
?
Thanks a lot!
If the previous condition was true doesn't this simply mean that ##g_{\mu\nu}^\prime## is the same function as ##g_{\mu\nu}##? Should we ask for:A metric ##g_{\mu\nu}## is said to be form-invariant under a given coordinate transformation ##x\to x^\prime##, when the transformed metric ##g^\prime_{\mu\nu}(x^\prime)## is the same function of its argument ##x^{\prime\mu}## as the original metric ##g_{\mu\nu}(x)## was of its argument ##x^\mu##, that is,
\begin{equation}
g^\prime_{\mu\nu}(y)=g_{\mu\nu}(y) \; \text{ for all }y.
\end{equation}
\begin{equation}
g^\prime_{\mu\nu}(x^\prime)=g_{\mu\nu}(x)
\end{equation}
?
Thanks a lot!