Black Hole Event Horizon: Beyond Schwarzschild Radius?

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Discussion Overview

The discussion centers on the properties of black holes, specifically whether there exist metrics in which black holes do not have a Schwarzschild radius. Participants explore the nature of event horizons in various black hole solutions, including stationary and non-stationary cases.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Exploratory

Main Points Raised

  • Some participants inquire about the possibility of black holes having event horizons that do not follow the form of a constant multiplied by mass.
  • It is noted that the event horizon of a rotating black hole, such as the Kerr-Newman solution, depends on both mass and angular momentum, challenging the idea that it is solely proportional to mass.
  • One participant asserts that the Kerr-Newman solution is the most general stationary solution that maintains the property of a radius proportional to mass.
  • Others argue that the Schwarzschild solution is a special case and that there are more general solutions, including dynamic black holes that do not conform to the Schwarzschild radius property.
  • Some participants mention specific metrics, such as the Vaidya metric, which may exhibit different properties regarding event horizons.
  • There is a discussion about the inner horizon of Kerr black holes, with claims that its size is not directly proportional to mass and that it can shrink under certain conditions.
  • Clarifications are made regarding the definitions of event horizons and Schwarzschild radii in the context of different black hole solutions.

Areas of Agreement / Disagreement

Participants express differing views on the properties of black holes and the applicability of the Schwarzschild radius. There is no consensus on whether all black holes must have an event horizon proportional to mass, with multiple competing perspectives presented.

Contextual Notes

Some participants highlight the limitations of existing definitions and the need for careful consideration of the assumptions involved in different black hole metrics. The discussion includes references to specific mathematical formulations and conditions that affect the properties of black holes.

Who May Find This Useful

This discussion may be of interest to those studying general relativity, black hole physics, and the mathematical properties of different black hole solutions.

Andru10
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Are there any known metrics in which black holes do not have the Schwarzschild radius? Specifically, I'm interested in whether it's possible for a black hole to have an event horizon which is not of the form: constant * mass.
 
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Andru10 said:
Are there any known metrics in which black holes do not have the Schwarzschild radius? Specifically, I'm interested in whether it's possible for a black hole to have an event horizon which is not of the form: constant * mass.
The event horizon for a rotating black hole does not only depend on the mass but also on the angular momentum.
 
Specifically, I'm interested in whether it's possible for a black hole to have an event horizon which is not of the form: constant * mass.
No. The most general black hole is represented by the Kerr-Newman solution, and it has this property.
 
Kerr-Newman don't have the property that the radius is proportional to the mass times a constant. It depends on both the angular momentum(as passionflower said) and the charge.

Also Kerr-Newman is not the most general black hole. It is only the most general stationary solution to the Einstein-Maxwell equations in four dimensions. There are obviously many more general solutions like for example time dependent ones with matter falling to the horizon.

The Schwarzschild solution is a very very special case.
 
Finbar said:
Kerr-Newman don't have the property that the radius is proportional to the mass times a constant. It depends on both the angular momentum(as passionflower said) and the charge.

The OP asked if there are black holes which do not have a schwarzchild radius i.e. r = 2GM. The kerr - newman solution is the most general stationary solution that DOES have this property.
 
WannabeNewton said:
The OP asked if there are black holes which do not have a schwarzchild radius i.e. r = 2GM. The kerr - newman solution is the most general stationary solution that DOES have this property.

No, for a kerr black hole
r = M + \sqrt{M^2-a^2}


in units G=1 where a = J/M and J is angular momentum.

Go read a book!
 
Finbar said:
No, for a kerr black hole
r = M + \sqrt{M^2-a^2} in units G=1 where a = J/M and J is angular momentum.

Go read a book!

That is a definition of r to find the location of the horizon in the kerr geometry i.e. at g_{rr} = \infty. This has nothing to with the fact that r = 2M IS the schwarzchild radius for a kerr black hole.
 
Last edited:
No, for a kerr black hole r = M + √(M2 - a2)
The point is that a is restricted to the range 0 < a < M, so M < r < 2M. The inner horizon is no longer spherical, but its size is proportional to M. In fact this must be the case, since M is the only parameter in the solution that sets the scale.
 
WannabeNewton said:
That is a definition of r to find the location of the horizon in the kerr geometry i.e. at g_{rr} = \infty. This has nothing to with the fact that r = 2M IS the schwarzchild radius for a kerr black hole.

r=2M has nothing to do with the event horizon of a Kerr black hole.

The OP asked whether the event horizon of a black hole is proportional to the mass times a constant. This is only the case for schwarzschild black hole.
 
  • #10
Bill_K said:
The point is that a is restricted to the range 0 < a < M, so M < r < 2M. The inner horizon is no longer spherical, but its size is proportional to M. In fact this must be the case, since M is the only parameter in the solution that sets the scale.

The inner horizon radius is not proportional to the mass either. Take fix J and take M large and the inner horizon shrinks to zero as J/M goes to zero.

a is not restricted to a<M. a>M is a naked singularity.
 
  • #11
Finbar said:
r=2M has nothing to do with the event horizon of a Kerr black hole.

The OP asked whether the event horizon of a black hole is proportional to the mass times a constant. This is only the case for schwarzschild black hole.

Yes excuse me I see what you are saying. g_{rr} = \infty and g_{tt} = 0 for a schwarzchild black hole is r = 2m but for a kerr black hole the actual horizon (not the ergosphere) g_{rr} = \infty is when \Delta = 0. Thanks mate; indeed I was mixing up the terms for the event horizon and the definition of schwarzchild radius.
 
  • #12
Andru10 said:
Are there any known metrics in which black holes do not have the Schwarzschild radius? Specifically, I'm interested in whether it's possible for a black hole to have an event horizon which is not of the form: constant * mass.

When "mass" is suitably defined, there are dynamic (non-stationary; no exterior timelike killing vector) black hole spacetimes that don't have this property. For an example that uses the Vaidya metric, see section 5.1.8 on page 132 (pdf page 148) of Eric Poisson's notes,

http://www.physics.uoguelph.ca/poisson/research/agr.pdf,

which evolved into the excellent book, A Relativist's Toolkit: The Mathematics of black hole Mechanics.

In this example, the apparent horizon has this property, but (a portion of) the event doesn't.
 
  • #13
Finbar said:
Kerr-Newman don't have the property that the radius is proportional to the mass times a constant. It depends on both the angular momentum(as passionflower said) and the charge.

Also Kerr-Newman is not the most general black hole. It is only the most general stationary solution to the Einstein-Maxwell equations in four dimensions. There are obviously many more general solutions like for example time dependent ones with matter falling to the horizon.

The Schwarzschild solution is a very very special case.

I would appreciate if you had any good links to the subject "Kerr-Newman is not the most general black hole"

I am interested in black holes where a lot of material is falling in from close to the top and bottem of the spinning black hole. Mostly in 3D aspects as I find many references and drawings on the internet really only seem to be 2D in nature (the axis of rotation is not precessing).
 
  • #14
Finbar said:
Also Kerr-Newman is not the most general black hole. It is only the most general stationary solution to the Einstein-Maxwell equations in four dimensions. There are obviously many more general solutions like for example time dependent ones with matter falling to the horizon.

edguy99 said:
I would appreciate if you had any good links to the subject "Kerr-Newman is not the most general black hole"

I am interested in black holes where a lot of material is falling in from close to the top and bottem of the spinning black hole. Mostly in 3D aspects as I find many references and drawings on the internet really only seem to be 2D in nature (the axis of rotation is not precessing).

I gave an example for non-spinning black holes in post #12.
 

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