How Can Two Black Holes Merge Within the Age of the Universe?

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The discussion centers on the paradox of how two black holes can merge within the universe's 14 billion-year age, given that matter falling into a singularity appears to take infinite time. Observers outside the event horizon never see matter cross it, yet the event horizons of two merging black holes can combine in finite time for an external observer. The merging process raises questions about the nature of event horizons and the time dilation experienced by observers near black holes. The conversation also touches on the implications of Hawking radiation and the complexities of different reference frames in understanding black hole mergers. Ultimately, the merging of black holes remains a fascinating topic that challenges our understanding of time and space in the context of general relativity.
Mordred
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THe universe is around 14 billion years matter falling into the singularity appear to take infinite time. So how would two black holes have had the time to complete a merger under those conditions? According to my understanding of GR we should be able to see mergers still in progress as the time reference at the event horizon and at the singularlity with itas infinite density would give us the apearance of infinite time taken which is well beyond the age of the Universe. Would the event horizon simply shift in size and encompass both singularities essentailly entailing two separate singularities inside one event horizon? If I recall Hawking radiation this process also takes a long time to reduce a large Black hole to nothing. So even if all the matter was pulled away from the smaller black hole to the larger, The smaller black hole would still not have had enough time to reduce to nothing. or am I correct in that last statement?
 
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An outside observer never sees matter cross the the event horizon. However, the event horizon itself responds approaching matter. As two collapsed stars with event horizon approach, their horizons merge in finite time for an external observer, with all matter of both stars still outside the merged event horizon.

Interestingly, if a planet approaches an event horizon, the horizon grows well before the planet reaches the horizon. The current event horizon reflects (in part) all matter that will eventually be trapped.
 
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The universe is around 14 billion years matter falling into the singularity appear to take infinite time.

And yet if you are falling with that matter, all takes place in "normal" (local) time.

Among the things Einstein brought to science is the understanding that there is no single "correct" frame of reference, all frames (observers) are "relative"...There is no universally correct observational frame...So what you see is likely different from what a distant observer sees.
 


Yeah I knew the part regarding normal time if your falling into the singularity, I was more interested in what we would see with the time dilation when we look at it from Earth.
 


PAllen said:
...As two collapsed stars with event horizon approach, their horizons merge in finite time for an external observer, with all matter of both stars still outside the merged event horizon.

Interesting. But what you call an event horizon is not an event horizon, but the potential event horizon should the entire matter of each star be within the horizon boundary.
 


Phrak said:
Interesting. But what you call an event horizon is not an event horizon, but the potential event horizon should the entire matter of each star be within the horizon boundary.

No, it really is the event horizon. The event horizon is defined against a total 4-manifold. It necessarily reflects the complete future history. The definition is the surface from which no light will escape to infinity. Imagine a light wave or photon so nearly trapped (assuming no more matter falls in) that it takes a thousand years to escape far from the event horizon. Now, assume in 800 years a baseball approaches the event horizon. This can be enough so the light never escapes. Without the baseball, this light would be just outside the event horizon. However, because a baseball will fall in 800 years from now, it is actually inside the event horizon.

I was also speaking of observers well outside the event horizon, so, as I said, no matter is ever seen to cross the growing event horizon.
 


PAllen said:
No, it really is the event horizon. The event horizon is defined against a total 4-manifold. It necessarily reflects the complete future history. The definition is the surface from which no light will escape to infinity. Imagine a light wave or photon so nearly trapped (assuming no more matter falls in) that it takes a thousand years to escape far from the event horizon. Now, assume in 800 years a baseball approaches the event horizon. This can be enough so the light never escapes. Without the baseball, this light would be just outside the event horizon. However, because a baseball will fall in 800 years from now, it is actually inside the event horizon.

I was also speaking of observers well outside the event horizon, so, as I said, no matter is ever seen to cross the growing event horizon.

I don't know what "800 years from now" means without reference to a coordinate chart.
 
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Phrak said:
I don't know what "800 years from now" means without reference to a coordinate chart.

I am referring, of course, to the 'egocentric coordinate system' (Fermi-Normal coordinates based on my world line).

Make a silly quibble, get a silly answer.

(Apologies to Sydney Coleman for use of egocentric frames).
 
  • #11


PAllen said:
I am referring, of course, to the 'egocentric coordinate system' (Fermi-Normal coordinates based on my world line).

Make a silly quibble, get a silly answer.

(Apologies to Sydney Coleman for use of egocentric frames).

Sorry if you think it's quibbling.

I don't think it is though. I take it that Fermi normal coordinates are those of a feely falling observer.

I believe I could define some coordinate system in which there are no event horizons forming, even aysmtotically. Then again, the event horizon is an artifact of Schwarzschild metric and not the Fermi metric. So we are talking about the coordinate singularity in one metric using the coordinates of another.
 
  • #12


Phrak said:
Sorry if you think it's quibbling.

I don't think it is though. I take it that Fermi normal coordinates are those of a feely falling observer.

I believe I could define some coordinate system in which there are no event horizons forming, even aysmtotically. Then again, the event horizon is an artifact of Schwarzschild metric and not the Fermi metric. So we are talking about the coordinate singularity in one metric using the coordinates of another.

I said several times already that I was speaking of observers distant from the horizon. Given that, it does not matter what coordinate system is used for the statements I made (as long as time is interpreted to be proper time, and the observer stays distant from the horizon and does not have extreme motion, which I thought goes without saying). By Fermi-normal coordinates I do not necessarily refer to a free falling observer. I mean you use a chosen worldline as time axis, and foliate spacetime with spacelike geodesics 4-orthogonal to this world line.

The event horizon singularity is coordinate dependent. The event horizon itself is a geometric feature of the manifold. A given null geodesic either reaches spatial infinity or it does not. This is not coordinate dependent, thus the horizon is not coordinate dependent. Its shape as a 2-surface does dependent on how spacetime is foliated into spacelike hypersurfaces, but you can't get rid of it or change anything substantive about its properties.

(I really thought you were just being pedantic, rather than didn't understand or disagreed with what I was saying).
 

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