Falling into a black hole

In summary, "Falling into a black hole" explores the theoretical consequences and phenomena associated with crossing the event horizon of a black hole. It discusses the intense gravitational forces at play, the concept of spaghettification—where objects are stretched due to gravity differences—and the potential for time dilation. The piece highlights the limits of our understanding of physics in such extreme environments and the implications for space-time and the universe's structure.
  • #36
Tomas Vencl said:
May be, but fact is that exact metric for evaporating “black hole” is unknown, so claiming that “in an evaporating spacetime it does not take an infinite amount of coordinate time to cross the horizon in Schwarzschild-like coordinates” is at least based on aproximations and rather speculative.
It is true that I don't know the exact metric for an evaporating black hole. However, there are a few things that we can indeed say based on first principles.

Since it is a black hole there is an event horizon where timelike worldlines can enter but not exit, this is what defines a black hole instead of a white hole. When evaporation is finished there is no more event horizon, this is what defines the evaporation. Without loss of generality, assign the time of the evaporation event to be ##t_E##. Meaning, after ##t_E## there is no event horizon. All coordinate charts, by definition, are smooth and one-to-one, including the distant observer's Schwarzschild-like chart. So the crossing of the event horizon cannot be assigned a time coordinate ##t_C>t_E##. Therefore, indeed, it does not take an infinite amount of coordinate time to cross the horizon.
 
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  • #37
Dale said:
It is true that I don't know the exact metric for an evaporating black hole. However, there are a few things that we can indeed say based on first principles.

Since it is a black hole there is an event horizon where timelike worldlines can enter but not exit, this is what defines a black hole instead of a white hole. When evaporation is finished there is no more event horizon, this is what defines the evaporation. Without loss of generality, assign the time of the evaporation event to be ##t_E##. Meaning, after ##t_E## there is no event horizon. All coordinate charts, by definition, are smooth and one-to-one, including the distant observer's Schwarzschild-like chart. So the crossing of the event horizon cannot be assigned a time coordinate ##t_C>t_E##. Therefore, indeed, it does not take an infinite amount of coordinate time to cross the horizon.
Sure, but you are not sure (since we do not have exact metric) that your assumptions (event horizon + evaporation) are even together physically possible . So this could be similar like counting of number of angels on tip of the needle.
I can imagine that in case of evaporation instead of real black hole there can be different object (not so black hole :-) from distant perspective indistinguishable (but yes, this is speculation already).
 
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  • #38
Tomas Vencl said:
Sure, but you are not sure (since we do not have exact metric) that your assumptions (event horizon + evaporation) are even together physically possible . So this could be similar like counting of number of angels on tip of the needle.
I can imagine that in case of evaporation instead of real black hole there can be different object (not so black hole :-) from distant perspective indistinguishable (but yes, this is speculation already).
They are not my assumptions, they are the assumptions of the question.
 
  • #39
Dale said:
They are not my assumptions, they are the assumptions of the question.
OK, perhaps it would be fair to also inform the inquirer that the assumptions may not be realistic (which I clumsily tried without any successs to do in my second comment).
 
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  • #40
Tomas Vencl said:
I think that my claim can be rephrased for example that there is no horizon to cross
Then you are not talking about Hawking's original model, or indeed any model with an event horizon. You are talking about a model like the Bardeen black hole that I referenced previously. But, as I have already said, I don't think that kind of model is what the OP of this thread is asking about.
 
  • #41
Tomas Vencl said:
in some models with firewall also falling observer do not cross the horizon (similarly to mentioned fig.3 at arxiv article).
As I said in the other thread where that paper was discussed, I don't think Fig. 3 in that paper is valid for a "firewall" model. It claims to be describing an evaporating black hole, but it looks more like a diagram (in weird coordinates) of maximally extended Schwarzschild spacetime, with both a black hole and a white hole region, and some kind of weird thing in the middle. Whatever it is, I don't think it's relevant to the discussion in this thread.
 
  • #42
Tomas Vencl said:
OK, perhaps it would be fair to also inform the inquirer that the assumptions may not be realistic (which I clumsily tried without any successs to do in my second comment).
I think most of the posts in this thread before you came into it were doing that.
 
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  • #43
PeterDonis said:
Then you are not talking about Hawking's original model, or indeed any model with an event horizon. You are talking about a model like the Bardeen black hole that I referenced previously.………….…..I think most of the posts in this thread before you came into it were doing that.
Yes,you are right. I am leaving the discussion for now. Thank you and Dale for your ttime.
 
  • #44
@A.T. I have never seen that discussion of what lead Einstein to GR before - its very digestible, thanks, and has me hooked enough to download and read the entire text.
 
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