Hawking radiation versus the cosmic background

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Discussion Overview

The discussion revolves around the relationship between Hawking radiation and cosmic background radiation (CMBR) in the context of black holes (BHs). Participants explore whether the energy from CMBR can compensate for the energy lost through Hawking radiation, particularly focusing on different sizes of black holes and their behavior over time.

Discussion Character

  • Debate/contested
  • Exploratory
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that for black holes smaller than approximately 70 microns, Hawking radiation dominates, leading to a decrease in size, while larger black holes absorb more radiation and grow.
  • Others argue that large black holes do not decay immediately but instead grow due to absorbing radiation, with Hawking radiation eventually taking over after an extremely long time, estimated at around 10^80 years.
  • A participant questions whether there exists a mass threshold where CMBR accretion always exceeds Hawking radiation, suggesting a need for a quantitative analysis rather than qualitative statements about time scales.
  • Another participant mentions John Baez's assertion that reasonable-sized black holes are unlikely to grow large enough to avoid eventual evaporation, although this requires a nontrivial calculation to confirm.
  • Some participants express curiosity about the time scales involved, particularly whether the 10^80 years is measured by an Earth-bound clock or another reference frame.

Areas of Agreement / Disagreement

Participants generally agree that Hawking radiation and CMBR interact in complex ways, but multiple competing views remain regarding the implications for black hole growth and decay. The discussion does not reach a consensus on whether there exists a mass where CMBR always exceeds Hawking radiation.

Contextual Notes

Participants note that the CMBR is cooling as the universe expands, which may affect the dynamics of black hole accretion and evaporation. There are unresolved questions regarding the specific mass thresholds and the calculations needed to understand the interplay between these two phenomena.

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Is the cosmic backround radiation incident on a black hole sufficient to make up for the energy lost through Hawking radiation?

And what if we include the average energy flux from discrete objects like galaxies, as seen in intergalactic space?
 
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For BH's smaller than ~70 microns, Hawking radiation dominates and the BH will get smaller. For BH's larger than this, absorbing radiation dominates and the BH will get bigger.
 
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Vanadium 50 said:
For BH's smaller than ~70 microns, Hawking radiation dominates and the BH will get smaller. For BH's larger than this, absorbing radiation dominates and the BH will get bigger.

Does this mean that the big black holes out there don't decay and go pop but just get bigger?

Cheers
 
cosmik debris said:
Does this mean that the big black holes out there don't decay and go pop but just get bigger?

Cheers
Yes. For now. EVENTUALLY, Hawking radiation takes over and they get smaller and smaller. I've seen numbers like 10E80 years for total evaporation of big ones.
 
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phinds said:
I've seen numbers like 10E80 years for total evaporation of big ones.

I am curious - by an Earth bound clock, or by the clock of an observer free-falling into the hole, or some different clock?
 
Grinkle said:
I am curious - by an Earth bound clock, or by the clock of an observer free-falling into the hole, or some different clock?
Earth-bound. Not that the Earth will be around for anything more than a totally trivial portion of that time. Better to call it a co-moving observer (and if you don't know exactly what that means, look it up)
 
phinds said:
Yes. For now. EVENTUALLY, Hawking radiation takes over and they get smaller and smaller

Is that true in general? Remember, Hawking radiation doesn't win until the BH is hotter than the CMBR, and while it is absorbing all that CMB radiation it is cooling.
 
Vanadium 50 said:
Is that true in general? Remember, Hawking radiation doesn't win until the BH is hotter than the CMBR, and while it is absorbing all that CMB radiation it is cooling.
10E80 years is a LONG time, so yes.
 
phinds said:
10E80 years is a LONG time, so yes.

Yes, and it's absorbing radiation all this time, growing and cooling. Have you calculated that for a BH of any size it eventually evaporates? I suppose one could add for any time and any cosmology.

In short - can you show me a calculation or quantitative argument?
 
  • #10
Vanadium 50 said:
Yes, and it's absorbing radiation all this time, growing and cooling. Have you calculated that for a BH of any size it eventually evaporates? I suppose one could add for any time and any cosmology.

In short - can you show me a calculation or quantitative argument?
I don't have the calculation but I've seen that stat here several times. Eventually the CMB fades away, effectively, as does ALL radiation coming at a BH and Hawking Radiation takes over. Again, 10E80 is just a STAGGERINGLY long time.
 
  • #11
The CMB is cooling as the universe expands. It started out at something like 3000K some 13.2 billion years ago and is now down to about 2.7K. Compared to 10^80 years, 13.2 billion is utterly insignificant.
 
  • #12
gneil, you're right that the universe has a long time to cool. But by the same argument, the BH has a long time to accrete.

I'm not arguing 10^80 years is a short time. I am asking is there a mass so large that the CMBR accretion always exceeds Hawking radiation. Yes, both decrease with time, and yes, 10^80 years is a long time. My question is whether there exists a mass (and possibly a cosmology) where the two curves never cross. I am willing to believe there is, and I am willing to believe there isn't. But if possible, I'd like a more quantitative answer than "10^80 is big" or "I read somewhere".
 
  • #13
Vanadium 50 said:
gneil, you're right that the universe has a long time to cool. But by the same argument, the BH has a long time to accrete.

I'm not arguing 10^80 years is a short time. I am asking is there a mass so large that the CMBR accretion always exceeds Hawking radiation. Yes, both decrease with time, and yes, 10^80 years is a long time. My question is whether there exists a mass (and possibly a cosmology) where the two curves never cross. I am willing to believe there is, and I am willing to believe there isn't. But if possible, I'd like a more quantitative answer than "10^80 is big" or "I read somewhere".

I knew that John Baez had written about this, so I looked it, and, interestingly, found

"But it would take a nontrivial calculation to show that reasonable-sized black holes have no chance of getting this big. I think it's true, but I haven't done the calculation.

For now, let's assume it's true: all black holes will eventually shrink away and disappear — none of them grow big enough to stick around when it gets really cold."

Baez's essay ca be found at
http://math.ucr.edu/home/baez/end.html
 
  • #14
Thanks, George. Baez says that 10^32 solar masses is about the dividing line. There's no known process that produces BHs this size, but then again there's no known process that produces 70 um BHs either.
 

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