- #1
binbagsss
- 1,254
- 11
So in deriving the metric, the space-time can be foliated by homogenous and isotropic spacelike slices.
And the metric must take the form:
##ds^{2}=-dt^{2}+a^{2}(t)\gamma_{ij}(u)du^{i}du^{j}##,
where ## \gamma_{ij} ## is the metric of a spacelike slice at a constant t
QUESTION:
So I've read that:
1) Homogenity would be broken if the a(t) was taken outside the metric
2) By isotropicity there can be no cross-terms dtdx, dtdy, dtdz.
What I know:
homogenous means the same throughout - translationally invariant.
isotropic means the same in every direction - rotationally invariant.
But I'm struggling to see how 1) and 2) follow from this. As stupid as it sounds, I don't really see where time comes in when these properties are only on the spacelike slices.
Cheers.
And the metric must take the form:
##ds^{2}=-dt^{2}+a^{2}(t)\gamma_{ij}(u)du^{i}du^{j}##,
where ## \gamma_{ij} ## is the metric of a spacelike slice at a constant t
QUESTION:
So I've read that:
1) Homogenity would be broken if the a(t) was taken outside the metric
2) By isotropicity there can be no cross-terms dtdx, dtdy, dtdz.
What I know:
homogenous means the same throughout - translationally invariant.
isotropic means the same in every direction - rotationally invariant.
But I'm struggling to see how 1) and 2) follow from this. As stupid as it sounds, I don't really see where time comes in when these properties are only on the spacelike slices.
Cheers.