Crazymechanic said:
Now the math of GR breaks at singularities and we know that yet PeterDonis you keep saying that matter and time and etc ceases to exist at singularity
Just to be clear, I am saying that that is the classical GR prediction. I am not saying I believe that the classical GR prediction is necessarily correct. I personally think it isn't because I don't think infinite spacetime curvature is physically reasonable; I think once you get to the Planck scale (roughly, when the radius of curvature of spacetime is of the same order as the Planck length), some kind of new quantum gravity physics will take over. But that's just my opinion; it seems to be a fairly common opinion among physicists, but it's still just an opinion.
Crazymechanic said:
the math leads us nowhere when used about singularities
That's not really true. The math (meaning the math of classical GR as it stands) says that tidal gravity (spacetime curvature) increases without bound as the singularity is approached, just as the value of the function f(x) = 1/x increases without bound as x approaches zero. (Technically, the singularity itself, r = 0, is not part of spacetime, so we can't actually say what happens "at" it; we can only say what happens as it is approached.) There is nothing ill-defined or mathematically suspect about it at all. Whether it is physically reasonable is a separate question, but mathematically, it's perfectly valid.
Crazymechanic said:
when we say that something ceases to exist there should be an explanation because matter can't just disappear in 'thin air" and we all know that.
This is one of the reasons why many physicists think singularities are not physically reasonable. But it's not as simple as "matter can't disappear into thin air". The mathematical expression of that statement is that the Einstein tensor and the stress-energy tensor are covariantly conserved (their covariant derivatives are identically zero), and that's true all the way down to the singularity. The real issue is that a timelike worldline reaches the singularity in finite proper time (to be technically correct, since the singularity itself is not part of the spacetime--see above--we should say that the limit of the proper time to fall to a radius r, as r goes to zero, is finite); but some people think that's OK because spacetime curvature increases without bound as r goes to zero, which could mean that any object, even an "elementary particle", would eventually be crushed or stretched out of existence by the increasing curvature.
Crazymechanic said:
Thirdly elementary particles probably get very compressed at the singularity and something happens to them but what exactly we don't know.
Or they get stretched; as I said in a previous post, there is both tidal stretching and tidal compression. But you're correct that we don't know exactly what happens to elementary particles under these conditions. We don't know enough about what elementary particles are to know that, because we haven't probed them on small enough length scales, as I said in a previous post.
Crazymechanic said:
I guess the debate about the Event horizon and the question what's behind the doors is really a dead end for now on atleast because physics itself forbids us from exploring such places
No, it doesn't forbid us from exploring them. It just forbids us from sending our results back out to be published in a journal.
Crazymechanic said:
even a quantum gravity theory no matter how good would not be the total answer because how do we know a theory is correct?
This is a good question too. Some physicists seem to think that when we discover the correct "theory of everything", we will somehow be able to prove mathematically that it *is* the theory of everything. Hawking, for example, likes to take that position in his popular books. I'm not sure how many other physicists believe that.