Proving the Existence of Event Horizon in Homogeneous Spacetimes

In summary, the conversation discusses the possibility of an event horizon disappearing in a Schwarzschild spacetime when the singularity due to a point mass is removed. The possibility is raised that this can be proven by examining the metric for the interior of stars with a homogeneous mass distribution and showing that there is no change in the timelike coordinate from t to r at any r. Other sources and discussions are suggested for further exploration of this topic.
  • #1
hellfire
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Consider a Schwarzschild spacetime. If the singularity due to the point mass is removed (e.g. with an homogeneous matter distribution), does the event horizon disappear? If yes (I assume this is the case), how can be proven that there exists no event horizon if there is no singularity? May be it is enough to show that in the metric for the interior of stars (with homogeneous mass distribution) there is no change of the timelike coordinate from t to r at any r, as in case of the vacuum Schwarzschild solution for r = 2GM (Schutz p. 290)? I was not able to find an expression for the metric of the interior of stars to check this.
 
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  • #2
There's an analysis of the metric of a star with a constant density rho online

http://www.pma.caltech.edu/Courses/ph136/yr2002/chap25/0225.1.pdf

It's very detailed and long, being a chapter from a textbook, you'll probably have to print out & study it to get very far.

The same results are also in MTW's gravitation. This topic came up late in the thread "The Mass of a Body" that you'll find here on Physics Forum, though I'm not sure if there will be anything useful in that discussion for your question.

I think another poster, DW, once posted some formulas about static stars as well, you might try searching the physics forum for that, too.

As far as the event horizon goes, I think the best test is to consider whether or not light can escape from an object. If there are null geodesics that connect the interior of the star to the exterior, it doesn't have an event horizon. [I haven't double-checked this definition though.]

[add]
I should clarify, there should always be ingoing null geodesics, but if there is a horizon, there won't be outgoing ones.
 
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  • #3
Thanks, pervect, I will take a look. Your proposal to consider the outgoing geodesics to prove whether an event horizon exists or not seams to be the best one, but I can imagine it may be difficult to do the calculations. What do you think about this possibility:

hellfire said:
May be it is enough to show that in the metric for the interior of stars (with homogeneous mass distribution) there is no change of the timelike coordinate from t to r at any r, as in case of the vacuum Schwarzschild solution for r = 2GM (Schutz p. 290)?
 
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FAQ: Proving the Existence of Event Horizon in Homogeneous Spacetimes

What is an event horizon?

An event horizon is the theoretical boundary around a black hole beyond which no light or matter can escape.

How is an event horizon related to singularity?

An event horizon is the result of the intense gravitational pull of a black hole's singularity, which is a point of infinite density and zero volume.

What happens at the event horizon of a black hole?

At the event horizon, the escape velocity (the speed required to escape the gravitational pull) becomes greater than the speed of light, making it impossible for anything to escape.

Can anything pass through the event horizon?

Once an object crosses the event horizon, it is pulled towards the singularity and cannot escape. However, some theories suggest that virtual particles can briefly exist inside the event horizon and then disappear.

How is the size of an event horizon determined?

The size of an event horizon is determined by the mass of the black hole. The more massive the black hole, the larger the event horizon will be.

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