How Fundamental Is General Relativity in Understanding Black Holes?

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SUMMARY

The discussion centers on the fundamental role of General Relativity (GR) in understanding black holes, specifically through the lens of the Schwarzschild metric, first derived in 1916. The Schwarzschild solution is a direct consequence of the complete Einstein field equations, G_uv = 8 pi T_uv, which relate spacetime curvature to matter density. The equivalence principle and special relativity (SR) contribute to the understanding of gravitational effects, such as time dilation, but cannot fully explain black hole properties. The evolution of black hole theories has shifted from viewing event horizons as singularities to recognizing them as coordinate system artifacts.

PREREQUISITES
  • General Relativity fundamentals
  • Einstein field equations (G_uv = 8 pi T_uv)
  • Schwarzschild metric
  • Equivalence principle and its implications
NEXT STEPS
  • Study the derivation of the Schwarzschild solution in detail
  • Explore the implications of the equivalence principle in gravitational fields
  • Investigate the differences between singularities and coordinate systems in GR
  • Examine modern interpretations of black holes and their event horizons
USEFUL FOR

Physicists, astrophysicists, and students of theoretical physics interested in the foundational aspects of General Relativity and its application to black hole research.

lalbatros
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Dear all,

The possibility of black holes can be traced back to a special solution of the Einstein's equations, the famous Schwarzschild metric in 1916.

I find this very impressive, since at that time, the GR was a very young theory and it would have been more than natural to be skeptic about such a solution and the theory that leads to this solution.

I would like to know which aspects of GR, which 'ingredients', are the root cause for the Schwarzschild solution and the discovery of black holes. Or in other words, how much of GR is needed to come to the idea of black holes.

Am I right to say that clocks slowing down in a gravitational field is a consequence of the equivalence principle and SR? And would it be right the say that black holes are the consequence of that in the limit of large gravitational fields? Could the Schwarzschild radius be derived from such a simple analysis, and how justified could it be?

Michel
 
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There was quite a bit of skepticism about black holes, and our understanding of them has improved considerably from the early days.

For instance, in some of the early papers, it was thought that the event horizon was a singularity of some sort, rather than an ill-behaved coordinate system. Also, early views of "black holes" tended to view them as "frozen stars".

To actually solve the metric for black holes, one needs the complete Einstein field equations, G_uv = 8 pi T_uv, that relate curvature to matter density.

I'm not sure how much one can derive about their proprerties using only the equivalence principle, unfortunately.
 

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