It's Official: Black Holes Have Lots Of Mass
KewlPC writes "Spaceflight Now reports in this article that some scientists have been able to measure the "weight" (yeah, yeah, it's actually mass, not weight) of a black hole that is (or was, 13 billion years ago) eating up the most distant known quasar, some 13 billion light years away."
Even I knew that. I mean, stuff keeps falling in them. You know that last significant figure to which they measured the weight? About 10^-8 percent of that are my keys, for sure.
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This is neat, I'd never heard of this before:
The extreme brightness of this quasar also shows that the black hole in its core is swallowing matter at the maximum rate possible. This maximum rate is called the "Eddington Limit". If the black hole were accreting matter any faster, it would shine even brighter, and the intense luminosity would actually exert enough pressure to stop any more material falling in.
So there's a limit / "max throughput" to how much matter a black hole can suck in? Very interesting.
they had to write out the long way how many zeroes a quadrillion had...
at least that's what I remember from astronomy classes. The article doesn't say if they take that into account or not - and if it's really so far away, that would be a lot of dust that light travelled through. If they do, they would have to assume some uniform amount of dust?
I'm curious as to whether black holes are compacted so much that most of the space between atoms (and even subatomic particles?) is gone, or whether the repulsions keeping them apart are even stronger than the force of the black hole's gravity.
Now that they have a measure of the weight, if they know anything about the density or the size, they've got the other value as well.
Just speculating, but since black holes do evaporate, and the smaller they are the faster they evaporate, I wonder what the implications of evaporation would be in the presense of an acretion disk.
Given that in the process of evaporation, a black hole emits radiation, at some point the radiation pressure from the evaporation would balance out the force of gravity pulling matter into the black hole so then the black hole might stabilize in size.
Surely they'll have named that limit already, but I don't think it's the same as the eddington limit.
Or perhaps there won't be a limit here because the cross section area of the acretion disk would be so small compared to the surface area of the event horizon. (yes, I think that incoming matter would have to form a disk and not form an acretion shell)
Atoms produce very specific patterns of absorption or emission in the light spectrum depending on species. A familiar example, is the solar spectrum, which is created by absorption of narrow bands in the spectrum by a large number of different elements in different states of ionization. Redshift causes the entire set of these lines to be moved towards the red end of the spectrum. They retain the spacing between themselves, so they can still be recognized in their new positions, and their new positions tell us how fast the object that created them is moving. Reddening caused by dust doesn't move these absorption lines. Instead it scatters light preferentially at the blue end of the spectrum, causing the entire end of that spectrum to dim, rather than creating narrow bands in it or moving narrow bands around. These two different processes are usually distinguishable.
"I'm so moist I'm sticking to the leather." -Kermit the Frog on The Late Late Show
What was all that about? Why not just say "the mass"? This is on a site that uses computer and physics jargon and acronyms all the time, mass isn't exactly an obscure concept.
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If you're talking about the radius of the event horizon, I believe that is proportional to the black hole's mass.
If you're talking about the physical size of the matter in the black hole, I don't know if that is something that can be measured. We'd have to find a way of getting data out out from below the event horizon. . .
You need it. The nearest star is Proxima Centauri at 4x10^13 km (also, your numbers for Alpha Centauri are erroneous). The 9 billion solar mass black hole's radius is thus .0225% of that distance.
"I'm so moist I'm sticking to the leather." -Kermit the Frog on The Late Late Show
One Quadrillion Earths is impressive and all, but let's stick to standard units people!
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The headline talks about "weighing" the black hole, so I used the word weight. But I knew I'd get reamed if I didn't mention that it's actually the mass of the black hole, not its weight, so I put that in there too. So much for hedging my bets.
But you're right. I should've written mass and left it at that.
...but I didn't even know they were Catholic!
IBM had PL/1, with syntax worse than JOSS,
And everywhere the language went, it was a total loss...
mks units (favored by many physicists):
G= 6.673x10^-11 N(m/kg)^2
cgs units (those wacky astronomers!):
G= 6.673x10^-7 dyne (cm/g)^2
"I'm so moist I'm sticking to the leather." -Kermit the Frog on The Late Late Show
That is a new low for Slashdot. An article about something which occurred 13 billions years ago?
What next? The weather forecast for the previous Big Bang?
Black hole evaporation is a slow process. It has essentially no effect on big black holes, and it isn't relevant to the eddington effect.
This timeline gives the birth of stars at occuring roughly 1 billion years after the big bang, which this article in January gives at between 11.2 and 20 billion years ago...
Wouldn't this hole place a lower limit of 14 billion years on the bang? And if last year's Hubble estimate of 13-14 billion years ago for the bang is right, wouldn't it pin it AT 14 billion years ago?
-T
-T
The article talks about a MgII line in the spectrum. Surely that's meant to be Mg++.
Graham
I doubt anybody is still reading this thread, but in case you are here is more information.
The above posts are correct that radiation pressure balances the force of gravity. But luminosity (the amount of radiation) goes up with mass way faster than gravity, so eventually the radiation pressure "wins" and the star gently blows apart. That provides an upper limit to normal stars. When I was taking stellar structure in grad school in the early 90's it was thought the limit is about 60 solar masses. Above that a star rapidly loses mass as radiation pressure carries the outer layers away.
There is a class of stars called Wolf-Rayet stars. They are extremely luminous blue supergiants that have masses in the 80-100 solar mass range. Interestingly, they all have enormously strong stellar winds and are losing mass at very high rates. In a very short time (astronomically speaking) they will drop to 60 solar masses, at which point we assume the Wolf-Rayet mechanism shuts down and the star becomes a "normal" 60 solar mass star.
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