Charles_Xu
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Why does the Schwarzschild metric have a singularity at r=0 if it is only valid outside the spherically symmetric static mass?
The Schwarzschild metric exhibits a singularity at r=0, which is significant in the context of black hole spacetimes. While the metric is valid outside a spherically symmetric static mass, the singularity arises when considering regions of gravitational collapse, as illustrated by the Oppenheimer-Snyder model from 1939. The Schwarzschild solution to the Einstein Field Equations (EFE) describes a vacuum solution where the stress-energy tensor is zero, meaning that the parameter M in the metric does not represent the mass of an object but rather characterizes the solution itself. Therefore, the singularity at r=0 is not included in the Schwarzschild manifold, which only applies to regions where r>0.
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If we are talking about the vacuum region outside a spherically symmetric static mass, that region does not include ##r = 0##, and it does not include a singularity.Charles_Xu said:Why does the Schwarzschild metric have a singularity at r=0 if it is only valid outside the spherically symmetric static mass?
The Schwarzschild solution to the EFE is vacuum everywhere - no mass anywhere, stress-energy tensor is zero everywhere, the ##M## that appears in the metric is a parameter that characterizes the solution not the mass of anything. Thus any point with ##r\gt 0## is an element of the manifold and it makes sense to consider the singularity at ##r=0##.Charles_Xu said:Why does the Schwarzschild metric have a singularity at r=0 if it is only valid outside the spherically symmetric static mass?
This is true but properly stating it was more work than I wanted to do.Dale said:Just to be slightly pedantic: the Schwarzschild manifold does not include r=0.