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Is there a theorem which proves that for a black hole to form, matter must gravitationally collapse to a singularity?
The defining property of a black hole is the event horizon and for the formation of an event horizon you do not need "matter to collapse to a singularity" (whatever you mean by this). For example imagine many stars arranged on a sphere with very large radius and centre Earth. They will fall towards us and an event horizon will form here and expand until it the shell of stars crosses it. And you will not notice anything until much later when the stars come here.Ranku said:Is there a theorem which proves that for a black hole to form, matter must gravitationally collapse to a singularity?
You can even make a black hole out of EM radiation, at least in theory - the word to look up is kugelblitz.Ranku said:Is there a theorem which proves that for a black hole to form, matter must gravitationally collapse to a singularity?
The singularity theorems (here the original one of Penrose) imply that a singularity will form if you have a trapped surface and the usual energy conditions are satisfied.Ibix said:You can even make a black hole out of EM radiation, at least in theory - the word to look up is kugelblitz.
A question that might be what the OP means (and I think is interesting anyway) is: do you have to have a singularity somewhere for an event horizon to exist? I think you do because you have to have a place other than ##\mathcal{I}^+## where light rays can terminate. I'm not sure how that's possible without a singularity somewhere in spacetime (noting @martinbn's comment that you can have an event horizon before the singularity exists). Or is there some topological oddity I'm not aware of?
One has to be careful here since the term "event horizon" is overloaded; the cosmological horizon in de Sitter spacetime, which is nonsingular everywhere, is also called an "event horizon". (The term is also used to describe the maximal future development of a comoving observer's past light cone in models like the best fit model of our current universe.)Ibix said:do you have to have a singularity somewhere for an event horizon to exist? I think you do
Please don't say that. A singularity is a mathematical concept, akin to a division by zero, not a physical one. Equations can become singular. "Where is this equation undefined" is a valid question, even if one cannot put the undefinedness into a box.martinbn said:imply that a singularity will form
My impression is that this "formation of singularity" is the standard terminology.Vanadium 50 said:Please don't say that. A singularity is a mathematical concept, akin to a division by zero, not a physical one. Equations can become singular. "Where is this equation undefined" is a valid question, even if one cannot put the undefinedness into a box.
Certainly no one will misunderstand what you’re saying.martinbn said:My impression is that this "formation of singularity" is the standard terminology.
The actual "singularity theorems", and more generally the global methods for analyzing spacetimes for which the canonical text is Hawking & Ellis, define "singularity" as geodesic incompleteness: there exist geodesics in the spacetime that cannot be extended past some finite value of their affine parameter. The concept of a singularity "forming" makes no sense in this formulation. The spacetime geometry doesn't "form"; it just "is".martinbn said:My impression is that this "formation of singularity" is the standard terminology.
And even that statement doesn't necessarily capture the real issue of geodesic incompleteness, since it is not as well understood as it should be that that is what "singularity" means in the actual mathematical framework in question.Nugatory said:life is too short to say “the solution of the EFE that we are considering has a singularity” every single time.
Let's put an observer on one of the stars.martinbn said:For example imagine many stars arranged on a sphere with very large radius and centre Earth. They will fall towards us and an event horizon will form here and expand until it the shell of stars crosses it. And you will not notice anything until much later when the stars come here.
Your understanding is incorrect.Bosko said:During the fall a shell of homogeneously distributed stars will reach the photon sphere.
What will the observer see?
According to my understanding: An infinite plane homogeneously filled with stars
Your humble opinion is wrong.Bosko said:If at that moment we let the observer calculate the force of gravitational pull of other stars on his star.
What will he get as a result?
Zero, in my humble opinion
This is incorrect.Bosko said:if the above mentioned stars are arranged so densely that they form a photon sphere, they will not fall towards the center due to gravity.
Both of these claims are incorrect. Your scenario is just a version of the model first investigated by Oppenheimer and Snyder in their classic 1939 paper. Both an event horizon and a singularity do form in that model.Bosko said:Neither an event horizon nor a central singularity will form.
Ok. What a star-filled photon sphere looks like to an observer from one of the stars?PeterDonis said:Your understanding is incorrect.
In Schwarzschild's solution there are two singularities ##r=0## and ##r=r_s##Vanadium 50 said:Boslo. Boslo. Bosko. Its OK not to know something. In that case, it may be more helpful to ask them in your own thtead than to chime in on someone else's. Try it! It works!
Your questions show that you think in non relativistic terms. This is not just wrong here it is meaningless. Before trying to understand black holes, horizons, singularities and so on you need to learn enough relativity.Bosko said:Ok. What a star-filled photon sphere looks like to an observer from one of the stars?
The meaning of the question is whether that sphere of stars will continue to fall and form an event horizon.
Will it continue to fall after that and end up in the central singularity.
There is no singularity at ##r=r_s##.Bosko said:In Schwarzschild's solution there are two singularities ##r=0## and ##r=r_s##
Your position is that: The central singularity is an imperfection of the mathematical model.
Do you think that the singularity ##r=r_s## is not a real singularity but a "wrong interpretation" of the solution?
If the stars were eternally hovering there, you would see an infinite number of them, yes, in a hall-of-mirrors kind of way. But they are not hovering - they are infalling at considerable speed. Because there's only flat spacetime inside the shell, you'd just see a Dopplered and aberrated sphere of stars everywhere below you. You might even see the sphere occupying some of the sky above you due to lightspeed delay, although I'm not 100% certain of that.Bosko said:Ok. What a star-filled photon sphere looks like to an observer from one of the stars?
Of course they'll continue to fall. What's going to stop them?Bosko said:The meaning of the question is whether that sphere of stars will continue to fall and form an event horizon.
Classically, the singularity isn't in the center, but it is where all the matter would end up. In reality, we expect GR to stop being accurate somewhere inside the horizon, so we don't know.Bosko said:Will it continue to fall after that and end up in the central singularity.
It's almost certainly a symptom of our model not being correct, true.Bosko said:Your position is that: The central singularity is an imperfection of the mathematical model.
It's a singularity in Schwarzschild's coordinate system, closely analogous to the issues with latitude and longitude at the poles - what's your longitude if you stand at the north pole? Just like the poles, there is no actual physical singularity there, and you can pick a different set of coordinates (Eddington-Finkelstein, Gullstrand-Painleve or Kruskal-Szekeres are well known ones) that are well behaved through the horizon.Bosko said:Do you think that the singularity ##r=r_s## is not a real singularity but a "wrong interpretation" of the solution?
They will see stars if they look in the tangential direction (along the photon sphere), including multiple images of stars (including their own) from light that has traveled around the photon sphere multiple times. But they will see empty space if they look radially inward or radially outward.Bosko said:What a star-filled photon sphere looks like to an observer from one of the stars?
Yes to both. But the answer to those questions has nothing whatever to do with how the stars look when the shell of stars has fallen inward to the photon sphere.Bosko said:The meaning of the question is whether that sphere of stars will continue to fall and form an event horizon.
Will it continue to fall after that and end up in the central singularity.
The one at ##r = r_s## is only a coordinate singularity. It has no physical meaning and it poses no issues with the model (just choose coordinates that don't have it).Bosko said:In Schwarzschild's solution there are two singularities ##r=0## and ##r=r_s##
No, it's not. The entire mathematical model is perfectly self-consistent. The locus ##r = 0## is not part of the mathematical model.Bosko said:Your position is that: The central singularity is an imperfection of the mathematical model.
It's a coordinate singularity. See above.Bosko said:Do you think that the singularity ##r=r_s## is not a real singularity but a "wrong interpretation" of the solution?