I cannot completely understand what is a regular method to solve Einstein's equations in GR when there are no handy hints like spherical symmetry or time-independence.
E.g. how can one derive Schwarzschild metric starting from arbitrary coordinates x0,x1,x2,x3? I don't even understand the stress-energy tensor form in such a case - obviously it should be proportional to δ(x−x0(s)), where x0(s) is a parametrized particle's world-line, but if the metric is unknown in advance how do I get x0(s) without any a priori assumptions?
No comments:
Post a Comment