- #1
davidge
- 554
- 21
In Weinberg's book it is said that a Static, Isotropic metric should depend on ##x## and ##dx## only through the "rotational invariants" ##dx^2, x \cdot dx, x^2## and functions of ##r \equiv (x \cdot x)^{1/2}##. It's clear from the definition of ##r## that ##x \cdot dx## and ##x^2## don't depend on the angular displacement. What I don't understand is why ##dx^2## is invariant under rotations, since it's the "pure" metric when written in spherical coordinates, and so it depends on the usual angles ##\theta## and ##\varphi##.