Black holes have been in the news a couple times recently.
On one end, there was the observation of an extremely large black hole in the early universe, when no black holes of the kind were expected to exist. My understanding is this is very much a “big if true” kind of claim, something that could have dramatic implications but may just be being misunderstood. At the moment, I’m not going to try to work out which one it is.
In between, you have a piece by me in Quanta Magazine a couple weeks ago, about tests of whether black holes deviate from general relativity. They don’t, by the way, according to the tests so far.
And on the other end, you have the coverage last week of a “confirmation” (or even “proof”) of the black hole area law.
The black hole area law states that the total area of the event horizons of all black holes will always increase. It’s also known as the second law of black hole thermodynamics, paralleling the second law of thermodynamics that entropy always increases. Hawking proved this as a theorem in 1971, assuming that general relativity holds true.
(That leaves out quantum effects, which indeed can make black holes shrink, as Hawking himself famously later argued.)
The black hole area law is supposed to hold even when two black holes collide and merge. While the combination may lose energy (leading to gravitational waves that carry energy to us), it will still have greater area, in the end, than the sum of the black holes that combined to make it.
Ok, so that’s the area law. What’s this paper that’s supposed to “finally prove” it?
The LIGO, Virgo, and KAGRA collaborations recently published a paper based on gravitational waves from one particularly clear collision of black holes, which they measured back in January. They compare their measurements to predictions from general relativity, and checked two things: whether the measurements agreed with predictions based on the Kerr metric (how space-time around a rotating black hole is supposed to behave), and whether they obeyed the area law.
The first check isn’t so different in purpose from the work I wrote about in Quanta Magazine, just using different methods. In both studies, physicists are looking for deviations from the laws of general relativity, triggered by the highly curved environments around black holes. These deviations could show up in one way or another in any black hole collision, so while you would ideally look for them by scanning over many collisions (as the paper I reported on did), you could do a meaningful test even with just one collision. That kind of a check may not be very strenuous (if general relativity is wrong, it’s likely by a very small amount), but it’s still an opportunity, diligently sought, to be proven wrong.
The second check is the one that got the headlines. It also got first billing in the paper title, and a decent amount of verbiage in the paper itself. And if you think about it for more than five minutes, it doesn’t make a ton of sense as presented.
Suppose the black hole area law is wrong, and sometimes black holes lose area when they collide. Even if this happened sometimes, you wouldn’t expect it to happen every time. It’s not like anyone is pondering a reverse black hole area law, where black holes only shrink!
Because of that, I think it’s better to say that LIGO measured the black hole area law for this collision, while they tested whether black holes obey the Kerr metric. In one case, they’re just observing what happened in this one situation. In the other, they can try to draw implications for other collisions.
That doesn’t mean their work wasn’t impressive, but it was impressive for reasons that don’t seem to be getting emphasized. It’s impressive because, prior to this paper, they had not managed to measure the areas of colliding black holes well enough to confirm that they obeyed the area law! The previous collisions looked like they obeyed the law, but when you factor in the experimental error they couldn’t say it with confidence. The current measurement is better, and can. So the new measurement is interesting not because it confirms a fundamental law of the universe or anything like that…it’s interesting because previous measurements were so bad, that they couldn’t even confirm this kind of fundamental law!
That, incidentally, feels like a “missing mood” in pop science. Some things are impressive not because of their amazing scale or awesome implications, but because they are unexpectedly, unintuitively, really really hard to do. These measurements shouldn’t be thought of, or billed, as tests of nature’s fundamental laws. Instead they’re interesting because they highlight what we’re capable of, and what we still need to accomplish.


Can you give some intuition about the reasoning behind the black hole surface theorem and why it is surprising? I am a mathematician with very limited knowledge of physics beyond what I learned in high school. However when I think about a Newtonian black hole it seems kind of obvious that the result of a merge of two black holes would have greater surface area then the earlier surfaces combined.
After all: the radius of the black hole is the distance from its center at which the escape velocity equals the speed of light (if I recall correctly). This means that it equals some positive constant A times its mass. Now the surface area of the black hole is some different positive constant B times its radius squared, so all in all we can say that the surface of a black hole with mass m equals Cm^2 for some third positive constant C.
You see where this is going. If two black holes of masses m_1 and m_2 merge, then before the merge the have a combined surface area of C(m_1^2 + m_2^2). After the merge, when all the dust settles, we have a spherical black hole of mass m_1 + m_2, which then has a surface area of C(m_1 + m_2)^2.
Obviously, obviously this is bigger than the original C(m_1^2 + m_2^2): the difference is Cm_1m_2 which is positive.
I guess things get more complicated when you take into account relativity, but can you shed some light on the question how?
BTW I have been a fan of your blog for a long time!
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ahem, I mean the difference is 2Cm_1m_2, which is even more positive than what I wrote…
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This is one of those things that is obvious in the simplest cases (non-rotating black holes in the Newtonian limit), but nontrivial to prove in the general case. Black holes emit gravitational radiation when they collide which transmits energy away, surface areas depend on both mass and angular momentum (and there are even two different horizons for Kerr black holes!), and energy isn’t conserved in general in GR anyway. So while two idealized black holes will obey the rule pretty easily, it took the ~40 years from Schwarzchild to Hawking for it to be proven that this happens in the general case.
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