- #1
- 321
- 64
Working through an online course "Introduction to General Relativity." They give the metric for, Kottler-Moller coordinates, i.e. $$ds^2=(1+ah)^2d\tau^2-dh^2-dy^2$$
and say that it "covers" the Rindler wedge in flat space time, which is defined by $$0<x<\infty,-x<t<x$$
I am having difficulty seeing precisely what it means for a metric to "cover" a region. Why doesn't the metric cover all of space-time? What is special about $$x=0$$ or $$t=0$$? Is there a singularity or degeneracy in the metric for some points?
and say that it "covers" the Rindler wedge in flat space time, which is defined by $$0<x<\infty,-x<t<x$$
I am having difficulty seeing precisely what it means for a metric to "cover" a region. Why doesn't the metric cover all of space-time? What is special about $$x=0$$ or $$t=0$$? Is there a singularity or degeneracy in the metric for some points?