Black Holes: Accretion Disks /Increase/ Angular Momentum?

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Discussion Overview

The discussion revolves around the relationship between accretion disks and the angular momentum of spinning black holes, particularly in the context of General Relativity (GR) versus classical mechanics. Participants explore how the angular momentum of a black hole may change as it accretes material from an accretion disk, raising questions about conservation laws and the dynamics involved.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that classical mechanics implies the total angular momentum should remain constant, while a GR description indicates that the system could end up with greater angular momentum.
  • Another participant counters that while GR complicates the calculation of angular momentum, it should still be conserved, noting that gravitational waves can carry away angular momentum in certain scenarios.
  • A later reply references Kip Thorne's work, indicating that gas accreting into a black hole can cause it to spin faster, questioning the mechanisms behind this phenomenon.
  • One participant introduces the idea that there may be residual angular momentum in the interstellar medium, suggesting that the initial conditions are not as straightforward as having zero angular momentum.

Areas of Agreement / Disagreement

Participants express differing views on the implications of GR for angular momentum conservation, with some asserting that it complicates the understanding while others maintain that conservation still holds. The discussion remains unresolved regarding the specific mechanisms that allow black holes to increase their angular momentum through accretion.

Contextual Notes

There are references to complex interactions in the accretion disk and the potential influence of gravitational waves, but these aspects are not fully explored or quantified in the discussion.

MattRob
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I've been reading Kip Thorne's "Black Holes and Time Warps," and it mentioned something rather counter-intuitive; apparently, when material forms an accretion disk and falls into a spinning black hole, it increases the angular momentum of it.

Now, let's take a gas cloud, and put a spinning black hole in it.

The gas cloud has zero angular momentum as a whole (L_{cloud} = 0), and the black hole itself has L_{hole} angular momentum.

From what I know of classical mechanics, the momentum of the system shouldn't change; once the black hole accretes all the gas of the cloud, it will, according to classical mechanics, spin slower, and the total momentum of the system will stay the same.

∑L_{final} = L_{cloud} + L_{hole} = L_{hole} = ∑L_{initial}
by classical mechanics.

So, am I understanding this correctly, that that classical mechanics' description of the system doesn't agree with General Relativity, and that a full GR description of the same spinning black hole and gas cloud will end with the entire system having more angular momentum?

∑L_{final} > L_{hole initial} + L_{cloud initial} = L_{hole initial} = ∑L_{initial}
by General Relativity.

If that's so, then how? The book didn't go into detail much on how that's the case, but I find it really odd/interesting and would like some insight on how it happens.
 
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So, am I understanding this correctly, that that classical mechanics' description of the system doesn't agree with General Relativity, and that a full GR description of the same spinning black hole and gas cloud will end with the entire system having more angular momentum?

No. The full GR description will make calculating the angular momentum much more problematical, though it can be defined in asymptotically flat space-times. But once you get over the hurdle of actually defining the angular momentum, it should be conserved. In some situations, such as inpiraling binaries, gravitational waves (GW) can carry away angular momentum, so you might have to add the GW angular momentum into the total to get a conserved number.
 
pervect said:
No. The full GR description will make calculating the angular momentum much more problematical, though it can be defined in asymptotically flat space-times. But once you get over the hurdle of actually defining the angular momentum, it should be conserved. In some situations, such as inpiraling binaries, gravitational waves (GW) can carry away angular momentum, so you might have to add the GW angular momentum into the total to get a conserved number.

Okay, I'm re-reading this bit again, I think my original bafflement confused me from understanding it properly...

For context, this portion of the book is on quasars and their discovery.
To quote;

How strong will the swirl of space be near the gigantic [black] hole? In other words, how fast will gigantic holes spin? James Bardeen deduced the answer: He showed mathematically that gas accreting into the hole from its disk should gradually make the hole spin faster and faster. By the time the hole has swallowed enough inspiraling gas to double its mass, the hole should be spinning at nearly its maximum possible rate - the rate beyond which centrifugal forces prevent any further speedup (Chapter 7). Thus, gigantic holes should typically have near-maximal spins.
-Black Holes and Time Warps by Kip Thorne

I guess my question then is simply how? There must be a lot of interesting interactions going on in the accretion disk in terms of GWs, then?
 
I haven't seen any detailed calculations, but my understanding is that there is some residual angular momentum in the interstellar media, it's not zero due to tiny imbalances. This is similar to the solar system, the sun and the planets all have nonzero spins, though the condensed gravitationally from the interstellar media. This process was rather similar in its major outline to the black hole case, t's just in the black hole case, the collapse radius is smaller, so the spin is faster.

The paper by Bardeen might have more info. I'm afraid I don't know much more possibly someone else can help.
 

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