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Scientists Discover Teeny Tiny Black Hole

Posted by Zonk on Wed Apr 02, 2008 06:04 PM
from the for-relative-terms-of-teeny-and-tiny dept.
AbsoluteXyro writes "According to a Space.com article, NASA scientists have discovered the smallest known black hole to date. The object is known as 'XTE J1650-500'. Weighing in at a scant 3.8 solar masses and measuring only 15 miles across, this finding sheds new light on the lower limit of black hole sizes and the critical threshold at which a star will become a black hole upon its death, rather than a neutron star. XTE J1650-500 beats out the previous record holder, GRO 1655-40, by about 2.5 solar masses."
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  • by Anonymous Coward on Wednesday April 02 2008, @06:05PM (#22945880)
    They say LHC-001 will be even smaller!

    (But who will be there to measure...?)
    • by sayfawa (1099071) on Wednesday April 02 2008, @06:52PM (#22946392)
      There may already be microscopic (more like picoscopic) black holes all around us. The thing with black holes is they are only dangerous if you get close to them. If they are small they can whiz right through us without hitting anything, much like many other particles that pass through us all the time. I'm not saying that creating one would be a good idea, but if, on the off-chance, one were created by the LHC it will probably be innocuous. I wish I could make those sound less like famous last words.
      • by ShadowBlasko (597519) on Wednesday April 02 2008, @07:03PM (#22946500) Homepage
        So thats where all my socks keep going!

      • Quantum Foam (Score:4, Informative)

        by jd (1658) <imipak@@@yahoo...com> on Wednesday April 02 2008, @09:09PM (#22947340) Homepage Journal
        There are going to be a near-infinite number of quantum-scale black holes and wormholes in whatever volume of space you care to imagine. They evaporate almost instantly. As for stellar black holes, the Chandrasaker Limit is 2.5 solar masses, with a relatively small margin of error. Absolutely nothing of interest will be learned until we're within 2.75 solar masses, because then we can define sensible confidence limits on what the value actually is.
        • Re:Quantum Foam (Score:5, Insightful)

          by rasputin465 (1032646) on Thursday April 03 2008, @04:58AM (#22949398)

          As for stellar black holes, the Chandrasaker [sic] Limit is 2.5 solar masses, with a relatively small margin of error.


          The value of the Chandrasekhar limit depends on how one performs the calculation, but typically it comes out to around 1.4 solar masses (not 2.5). But actually, this is not so much the interesting question, because the Chandrasekhar limit applies only to white dwarfs, whose mass is supported by electron degeneracy pressure [wikipedia.org]. This is only one type of a much broader concept called fermion degeneracy pressure.

          For example, a neutron star is much denser than a white dwarf, and is supported by neutron degeneracy pressure instead of electron degeneracy pressure and hence the Chandrasekhar limit does not apply to neutron stars. The equivalent limit for neutron degenerate matter is called the Tolman-Oppenheimer-Volkoff limit [wikipedia.org]. Like the Chandrasekhar limit, this calculation is very dependent on the behavior of the degenerate matter, but UNlike the Chandrasekhar limit, we know very little about the properties of neutron degenerate matter, and so the uncertainty of the T-O-V limit is quite large; it is usually placed (as you can see in the wikipedia article that I link to) between 1.5 and 3.0 solar masses. And there are even denser objects that have been proposed (though not observed) made of quark degenerate matter, and the limit on the mass of these things is even more uncertain.

          So the point is, there is still a good deal of physics that can come from the observation of a 3.8 solar mass black hole, as it can constrain various models of fermion degenerate matter.
      • I'm not saying that creating one would be a good idea, but if, on the off-chance, one were created by the LHC it will probably be innocuous. I wish I could make those sound less like famous last words.
        What would be really scary is if the chief scientist says "Hold my beer and watch this" just before pushing the master ignition switch...
      • Re: (Score:3, Interesting)

        The tidal effects would cause some damage. See the short story "Thw Hole Man" by Larry Niven.
      • by Kingrames (858416) on Wednesday April 02 2008, @10:41PM (#22947852)
        So what you're saying is that the odds of getting sucked into a black hole are proportional to its size. That sounds like something you could write a couple hundred to a couple thousand pages on and get a doctorate out of.

        But... it needs more string theory.
    • Re: (Score:3, Informative)

      Is it smaller than this one [newscloud.com]?
      Not even close, do you really think that we could make a 3.8 solar mass black hole in the lab (that's several hundred thousand times the mass of our planet)? A more accurate term for the kind of black hole we might make in the lab is the hypothetical "microsingularity".
  • by Anonymous Coward on Wednesday April 02 2008, @06:08PM (#22945924)
    HILARITY!
  • by cryptoluddite (658517) on Wednesday April 02 2008, @06:10PM (#22945948)
    I see we weren't the first to build a large hadron collider.
  • by Anonymous Coward on Wednesday April 02 2008, @06:14PM (#22945984)
    It may look cute now. But they grow up.
  • Size vs Age (Score:5, Interesting)

    by SKiRgE (411560) on Wednesday April 02 2008, @06:15PM (#22945996)
    While it may be possible that this black hole was formed from a relatively small (to form a black hole) star, couldn't it also be the case that it just a really old black hole? Hawkings told of how black holes can 'evaporate' over time with lack of surrounding matter, perhaps that could be the case here.
    • Possible, but I believe they evaporate over the course of trillions of years via Hawking radiation. Based on recent evidence, the universe is only old enough for it to still have been the smallest yet discovered.

      At least, if I were a scientist and not someone pulling this directly out of my ass, that might be what is happening here.
    • Re:Size vs Age (Score:5, Informative)

      by smolloy (1250188) on Wednesday April 02 2008, @06:32PM (#22946170)
      It is true that black holes will evaporate over time, but they will also gain mass from infalling matter.

      But!

      The temperature of a black hole can be defined by the rate at which Hawking photons are streaming away from it. In the case of a black hole of a few solar masses, this temperature will be in the nano-Kelvin (I think -- don't hurt me if I'm wrong by a few orders of magnitude). Now remember everything in the Universe is sitting in a bath of cold photons from the Big Bang (i.e. the microwave background). These photons have a temperature of ~4 Kelvin.

      Therefore, black holes whose Hawking temperature is above the microwave background will be net *gaining* mass.

      Which is all a long way of saying, no, this isn't a normal size black hole that has decayed over time. It must have been created at this mass (or smaller).

  • Goldilocks (Score:5, Funny)

    by Dopamine, Redacted (1244524) on Wednesday April 02 2008, @06:16PM (#22946016)
    So, we've now discovered the biggest and smallest black holes known to exist within about a week of each other.

    When we find the most average, space bears will come and blast us into porridge.

    Astronomy kicks ass.
  • untrue statement (Score:5, Interesting)

    by ILuvRamen (1026668) on Wednesday April 02 2008, @06:20PM (#22946056)
    They can't figure out the "critical threshold" because there isn't one. It all depends on too many variables to set a universal limit (hehehe get it...universal :-P) It depends on how much nuclear activity there is still going on when it start collapsing and what the amount of heavier atoms is and the amount of other things orbiting the star and any other forces affecting the star at that time and how fast it's moving and spinning. Mass is a smaller part of the calculation than they're making it sound like. If they're going to factor everything in just to find some minimum mass, well duh, two particles and a hell of a lot of force. Haven't they suggested that in that big particle accelerator aka donut of doom. So yeah, a critical mass threshold doesn't exist.
  • by syousef (465911) on Wednesday April 02 2008, @06:31PM (#22946162) Journal
    For those of you who haven't done any Astrophysics...

    http://en.wikipedia.org/wiki/Chandrasekhar_limit [wikipedia.org]
  • by nick_davison (217681) on Wednesday April 02 2008, @06:56PM (#22946432)

    "this finding sheds new light"
    I'm pretty sure it doesn't.
    • by Ecuador (740021) on Wednesday April 02 2008, @06:18PM (#22946032) Homepage
      While black holes is not my area, I can tell you that when someone talks about the size of the black hole, they refer to the event horizon, since you can't really measure anything going on inside it.
      The mass of the black hole is the most defining characteristic.
    • by Geoffrey.landis (926948) on Wednesday April 02 2008, @06:21PM (#22946064) Homepage

      I thought that Black Holes had no dimensions, but this one is several miles across. Where have I gone wrong?

      A black hole, conventionally, consists of an event horizon surrounding a region of space from which you can't send information to the external world. This region of space is not a point, it has a well-defined circumference. (Because of the non-euclidean nature of general relativity, it doesn't actually have a well-defined radius (since you can't measure across the middle!) but people usually just consider the radius as if it were defined as the circumference divided by 2 pi, and don't worry about the fact that you can't actually measure it.)

      At the center of the black hole is, according to general relativity, a point singularity, which indeed has no dimensions.

      • by The Only Druid (587299) on Wednesday April 02 2008, @07:01PM (#22946472)
        Actually, that's only true of a non-rotating (or Kerr) singularity. All natural black holes will be rotating (the black hole maintains the rotational momentum of the pre-collapse mass). In a rotating black hole, the singularity is actually a ring (or torus). Inside that ring/torus, there is a tear in space.

        It was this tear that lead, if I recall, to the original conjectures of a white hole, and the Einstein-Rosen bridge.
        • Actually, that's only true of a non-rotating (or Kerr) singularity.
          Yeah, I thought about mentioning that, and decided what I was writing was getting a bit complicated already

          All natural black holes will be rotating (the black hole maintains the rotational momentum of the pre-collapse mass).

          Well, maybe. Actually, rotating black holes radiate away angular momentum, and they also preferentially eat material that reduces their angular momentum, so it's an open question as to whether real black holes will be rotating. Probably, because the accretion disk is likely to be rotating, and it swallows up the accretion disk and gains the momentum from it, but I'm not sure you can necessarily say that all natural black holes will rotate.

          In a rotating black hole, the singularity is actually a ring (or torus). Inside that ring/torus, there is a tear in space.
          It was this tear that lead, if I recall, to the original conjectures of a white hole, and the Einstein-Rosen bridge.

          Actually, the Einstein-Rosen bridge comes from the maximum analytical extension of the Flamm embedding, way predating the Kerr solution. (It's a very trivial embedding, z = sqrt(r). The extension is z = plus or minus sqrt(r).) Turns out that the extended Flamm embedding is misleading, and a Schwartzschild black hole isn't a wormhole after all. But that wasn't obvious.

      • Re: (Score:3, Interesting)

        Actually, the Schwarzchild solution does have a well-defined radius. In fact, the problem is that it has many well-defined radii, depending on what you mean by the term (as you point out, this comes about because of the non-Euclidean nature of the geometry). The commonly quoted "Schwarzschild radius" r = 2GM/c^2 is obtained by taking the area of the horizon and figuring out which "r" you would have to plug into A = 4 pi r^2 [true for a flat space sphere] to get the right result. Taking the circumference an
        • by Geoffrey.landis (926948) on Wednesday April 02 2008, @08:23PM (#22947070) Homepage

          Actually, the Schwarzchild solution does have a well-defined radius.

          No, actually it doesn't. What is usually called the Schwartzschild "radius" is not actually a radius by the definition of the word, "distance to the center".

          In fact, the problem is that it has many well-defined radii, depending on what you mean by the term (as you point out, this comes about because of the non-Euclidean nature of the geometry). The commonly quoted "Schwarzschild radius" r = 2GM/c^2 is obtained by taking the area of the horizon and figuring out which "r" you would have to plug into A = 4 pi r^2 [true for a flat space sphere] to get the right result.

          Exactly. You can calculate the area (which is well defined) and divide it by 4 pi, and you are free to call that the radius if you like. Or, equivalently, divide the circumference by two pi. But you can't measure the distance to the center.

          Taking the circumference and dividing by 2 pi would achieve the same result. However, it is quite possible to figure out the proper distance between the horizon and the singularity by measuring the distance an infalling observer would travel. This distance is finite.

          Finite... and timelike. It would be a little like trying to define the radius of a circle if you're standing on the circumference, and the center is next Tuesday at noon.

          A problem can occur if you try and use constant time slices, using the "natural" time coordinate as defined by an observer far from the black hole. This gives silly results, but that is only because of badly behaved coordinates.

          Within the event horizon, any choice of coordinates is rather badly behaved, because there is no well-behaved stationary coordinate system.

        • Re: (Score:3, Interesting)

          it doesn't actually have a well-defined radius (since you can't measure across the middle!)

          Why do you need to measure *across* the middle to measure the radius?

          Is there a (theoretical) problem with using some kind of high tech space calipers to measure the radius without going anywhere near the 'middle'?

          You could, but the result wouldn't really be right. A black hole is like that blessed +2 bag of holding that has much more room inside it than the space that it actually encompasses. I never really studied general relativity, but I think that when an object is in a strong gravity field, it becomes shorter (or everything else becomes longer). This means that the notion of length gets a bit weird. Similarly, if you used calipers to measure the diameter of a block hole, the sides of the calipers would no long

        • Re: (Score:3, Interesting)

          Is there a theoretical way to revert a singularity?
          In theory, they radiate themselves out of existence over time through Hawking Radiation [wikipedia.org]. They constantly release energy, which reduces their mass. If they lose more mass than they swallow, then their event horizon will shrink. Eventually, there'll be no mass left, and no black hole.
    • Re: (Score:3, Informative)

      Would it be more correct to say this is a measurement of the event horizon?

      Yes that's what astronomers mean when they say how "big" a black hole is.
    • Re: (Score:3, Interesting)

      What is the theoretical time before this black hole evaporates through Hawking radiation?
      • What is the theoretical time before this black hole evaporates through Hawking radiation?

        About 10^68 yr. Bring a book.

        Bemopolis
      • Re: (Score:3, Insightful)

        INfinite.

        A black hole of any stelar size will only radiate like a body in the femto-kelvin range.

        This means that galactic background radiation will "refill" it more than it could ever lose.
    • by Anonymous Coward on Wednesday April 02 2008, @07:11PM (#22946560)
      ok, I am ripping most of the info from here: http://www.physicsforums.com/showthread.php?t=122375&page=6 [physicsforums.com]

              "If they were able to make a small blackhole, and it got "loose" and fell to the center of the Earth, the pressures at the Earths core would force material into it so fast that even a very small one would gobble us up very fast. I am not sure what the exact pressure is at the Earths core but it could force material through even a very small "hole" very quickly. I do agree that once it gobbled up the Earth, it would just continue to orbit the Sun, and the Moon would still orbit the blackhole as if it were the Earth..."

      No, you should read this thread.

      First of all, a black hole that falls to the center of the earth, wouldn't stop there, but would continue falling up on the other side, just to plunge in again, and on and on, because there's no "friction" on the black hole.

      Second, there have been posted in this thread a lot of calculations of the speed at which it would gobble up matter.
      Don't forget that the black hole we're talking about here IS MUCH MUCH SMALLER THAN A PROTON. As such, pressures on *atomic* level (such as in the center of the earth) matter little: the black hole travels most of the time in the empty space between nucleae.
      A way to calculate the probability of hitting a nucleus (and somehow imagining that it would gobble up the entire nucleus, which is MUCH MUCH bigger than the black hole itself - which is a worst-case scenario) is done by calculating the "cross section" of the black hole and its probability to cross a nucleus on its voyages through the earth. We know its speed (just falling), and knowing the cross section and the density of nucleae, we can estimate how many nucleae it could eat per unit of time.

      For a classical black hole, the calculation is done in the link provided by Pervect in this post:
      http://www.physicsforums.com/showpos...4&postcount=12 [physicsforums.com]

      for a MUCH LARGER black hole, about the size of a proton, weighting a billion tons (figure that! A black hole *the size of a proton* weights a billion tonnes ; we're talking here about black holes that weight 10 TeV or 10^(-24) kg - go figure how small it is !)

      For more exotic calculations which are more severe, orion made some, and arrived at a time to eat the earth ~ 10^46 years.

      All this in the following rather un-natural hypotheses:
      - no Hawking radiation (which would make the black hole evaporate almost immediately)
      - production of black hole EXACTLY IN THE CENTER OF GRAVITY of the collision (no remnant particles)
      - very high production rate, producing billions of black holes per second.

      I am not a physicist, but from what little physics I have had, and from reading threw the thread/flamewar, I dont think we have to worry about the LHC