Black hole
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of hot plasma orbiting a black hole (from NASA)]]A classical black hole is a theoretical concentration of mass with a gravitational field so strong that its escape velocity exceeds the speed of light. This implies that nothing, even light can escape its gravity, hence the term black. The name black hole is very widespread, even though the theory does not refer to any hole in the usual sense.
According to classical general relativity, no matter or information can flow from the interior of a black hole to an outside observer (e.g. one cannot bring out some of its mass, or light it up with a light source such as a flashlight, or retrieve any information about the material that has entered the black hole), although quantum mechanics may allow deviations from this strict rule. The existence of black holes in the universe is well supported both theoretically and by astronomical observation; however, a small minority of physicists dissent.
History
The concept of a body so massive that not even light could escape from it was put forward by the British geologist John Michell in a 1783 paper sent to the Royal Society. At that time, the Newtonian theory of gravity and the concept of escape velocity were well known. Mitchell computed that a body 500 times the radius of the Sun and of the same density would have at its surface an escape velocity equal to the speed of light, and therefore would be invisible. In his words:
- If the semi-diameter of a sphere of the same density as the Sun in the proportion of five hundred to one, and by supposing light to be attracted by the same force in proportion to its mass with other bodies, all light emitted from such a body would be made to return towards it, by its own proper gravity.
In 1796, the French mathematician Pierre-Simon Laplace promoted the same idea in the first and second edition of his book Exposition du Systeme du Monde. It disappeared in later editions. The whole idea gained little attention in the 19th century, since emphasis was put on the wave properties of light, which were thought not to be influenced by gravity.
In 1915 Einstein developed the theory of gravity called General Relativity. Earlier he had shown that gravity does influence the wave properties of light. A few months later Karl Schwarzschild gave the solution for the gravitational field of a point mass, showing that something we now call a black hole could theoretically exist. The Schwarzschild radius is now known to be the radius of a black hole, but was not well understood at that time. Schwarzschild himself thought it not to be physical.
In the 1920s, Subrahmanyan Chandrasekhar argued that special relativity demonstrated that a non-radiating body above a certain mass, now known as the Chandrasekhar limit, would collapse since there would be nothing that could stop the collapse. His arguments were opposed by Eddington, who believed that something would inevitably stop the collapse.
In 1939 Oppenheimer and H. Snyder predicted that massive stars could undergo a dramatic gravitational collapse. Black holes could in principle be formed in nature. Such objects for a while were called frozen stars since the collapse would be observed to rapidly slow down and become heavily reddened near the Schwarzschild radius. However, these hypothetical objects were not the topic of much theoretical interest until the late 1960s.
Interest in collapsed objects was rekindled in 1967 with the discovery of pulsars. Shortly thereafter, the use of the expression "black hole" for this concept was coined by theoretical physicist John Wheeler [1].
Qualitative physics
A correct understanding of black holes is possible only within the framework of general relativity, the most modern theory of gravitation.The event horizon
The "surface" of a black hole is the so-called event horizon, an imaginary spheroidal surface surrounding all the hole's mass. The event horizon bounds the "interior" of the black hole; anything there, including photons directed outwards, are prevented from reaching the event horizon by the strong gravitational field. On the other hand, particles from outside that region can fall in and cross the event horizon, but will never be able to leave.Since no particles can leave the interior, there is no way of sending information from inside the event horizon to an observer outside it. Black holes have no observable external characteristics that can be used to determine what they are like inside. According to classical general relativity, black holes can be entirely characterized according to three parameters: mass, angular momentum and electric charge, a principle summarized by the saying "black holes have no hair".
Objects in a gravitational field experience a slowing down of time, called time dilation. This phenomenon has been verified experimentally in the Scott Rocket Experiment of 1976 [1]. Near a black hole, the time dilation increases to a large degree. From the point of view of an external observer, it appears to take an infinite amount of time for an object to approach the event horizon, at which point it is infinitely red-shifted. But although the light from an infalling object crossing the event horizon will take an infinite amount of time to reach a distant observer, from the point of view of the object itself it will take a finite time to cross the event horizon and reach the singularity.
The singularity
At the center of the event horizon is a singularity, a place where general relativity predicts that spacetime becomes infinitely curved (i.e., where gravity becomes infinitely strong). Spacetime inside the event horizon is peculiar in that the singularity is literally the only possible future, so all particles within the event horizon must move inexorably towards it (Penrose and Hawking [1]).It is expected that future refinements or replacements of general relativity (in particular quantum gravity) will change what is thought about the nature of black hole interiors. Most theorists interpret the mathematical singularity of the equations as indicating that the current theory is not complete, and that new phenomena must come into play as one approaches the singularity.
Falling in
Consider a hapless astronaut falling radially towards the center of a simple Schwarzschild-type (non-rotating) black hole. The closer he gets to the event horizon, the longer the photons he emits take to escape from the black hole's gravitational field. A distant observer will see the astronaut's descent slowing as he approaches the event horizon, which he never appears to reach. (Actually, the astronaut will become effectively invisible due to red-shifting. Detectors do not exist that can "see" wavelengths longer than a few meters.)However, in his own frame of reference, the astronaut will cross the event horizon and reach the singularity, all in a finite amount of time. Once he has crossed the event horizon he can no longer be observed from the outside universe. As he falls, he will notice his feet, then his knees, becoming increasingly red-shifted until they appear invisible. As he nears the singularity, the gradient of the gravitational field from head to foot will become considerable, and he will feel stretched, and finally torn. This gradient becomes large enough, close to the singularity, to tear atoms apart. The point at which these tidal forces become fatal depends on the size of the black hole. For a very large black hole such as those found at the center of galaxies, this point will lie well inside the event horizon, so the astronaut may cross the event horizon painlessly. Conversely, for a small black hole, those tidal effects may become fatal long before the astronaut reaches the event horizon.
Rotating black holes
According to theory, the event horizon of a black hole that is not spinning is spherical, and its singularity is (informally speaking) a single point. If the black hole carries angular momentum (inherited from a star that is spinning at the time of its collapse), it begins to drag space-time surrounding the event horizon. This spinning area surrounding the event horizon is called the ergosphere and has an ellipsoidal shape. Since the ergosphere is located outside the event horizon, objects can exist within the ergosphere without inevitably falling into the hole. However, because space-time itself is moving in the ergosphere, it is impossible for objects to remain in a fixed position. Objects grazing the ergosphere could in some circumstances be catapulted outwards at great speed, extracting energy (and angular momentum) from the hole, hence the name ergosphere because it is capable of doing work.Entropy and Hawking radiation
In 1971, Stephen Hawking showed that the total event horizon area of any collection of classical black holes can never decrease. This sounded remarkably similar to the Second Law of Thermodynamics, with area playing the role of entropy. Therefore, Bekenstein proposed that the entropy of a black hole really is proportional to its horizon area. In 1975, Hawking applied quantum field theory to a semi-classical curved spacetime and discovered that black holes can emit thermal radiation, known as Hawking radiation. This allowed him to calculate the entropy, which indeed was proportional to the area, validating Bekenstein's hypothesis. It was later discovered that black holes are maximum-entropy objects, meaning that the maximum entropy of a region of space is the entropy of the largest black hole that can fit into it. This led to the proposal of the holographic principle.Hawking radiation originates just outside the event horizon and (semi-classically) does not carry information from its interior. However, this means that black holes are not completely black. Moreover, the effect implies that the mass of a black hole slowly evaporates with time. Although these effects are negligible for astronomical-sized objects, they are significant for very small black holess where quantum mechanical effects dominate. Indeed, small black holes are predicted to undergo runaway evaporation and will therefore eventually vanish in an burst of radiation. Hence, every black hole that cannot consume new mass has a finite life that is directly related to its mass.
On 21 July 2004 Stephen Hawking presented a new argument that black holes do eventually emit information about what they swallow, reversing his previous position on information loss. He proposed that quantum perturbations of the event horizon could allow information to escape from a black hole, where it can influence subsequent Hawking radiation [1]. The theory is still undergoing review, and if it is accepted it is likely to resolve the black hole information paradox. In the mean time, the announcement has attracted a lot of attention in the media.
Reality of black holes
Do black holes exist?
General relativity (as well as most other metric theories of gravity) not only says that black holes can exist, but in fact predicts that they will be formed in nature whenever a sufficient amount of mass gets packed in a given region of space, through a process called gravitational collapse. As the mass inside that region increases, its gravity becomes stronger — or, in the language of relativity, the space around it becomes increasingly deformed. When the escape velocity at a certain distance from the center reaches the speed of light, an event horizon is formed within which matter must inevitably collapse onto a single point, forming a singularity.A quantitative analysis of this idea led to the prediction that a star with about 3 times the mass of the sun will almost inevitably reach a point in its evolution where, having exhausted all its nuclear fuel, it will shrink to the critical size needed to undergo gravitational collapse. Once it starts, the collapse cannot be stopped by any physical force, and a black hole is created. Thus, to the question "do black holes exist", astrophysists generally answer "most likely" — but admit that no definite proof exists yet.
A few physicists, claiming to follow the Einsteinian point of view, believe that such black holes do not exist, because some process, like the Fifth Force, will stop the collapse. However, this conjecture requires some radically new and untested physics (antigravity).
Stellar collapse will generate black holes containing at least one or two solar masses. Black holes smaller than this limit can only be created if their matter is subjected to sufficient pressure from some source other than self-gravitation. The enormous pressures needed for this are thought to have existed in the very early stages of the universe, possibly creating primordial black holes which could have have masses smaller than that of the sun.
Supermassive black holes containing millions to billions of solar masses could also form wherever a large number of stars are packed in a relatively small region of space, or by large amounts of mass falling into a "seed" black hole, or by repeated fusion of smaller black holes. The necessary conditions are believed to exist in the centers of some (if not most) galaxies, including our own Milky Way.
Can they be discovered?
Theory says that we cannot detect black holes by light that is emitted or reflected by the matter inside them. However, those objects can be detected from observation of phenomena near them, such as gravitational lensing and stars that appear to be in orbit around space where there is no visible matter.The most conspicuous effects are believed to come from matter falling into a black hole, which (like water flowing into a drain) is predicted to collect into an extremely hot and fast-spinning accretion disk around the object before being swallowed by it. Friction between adjacent zones of the disk causes it to become extremely hot and emit large amounts of X-rays. This heating is extremely efficient and can convert about 50% of the mass energy of an object into radiation, as opposed to nuclear fusion which can only convert a few percent of the mass to energy. Other predicted effects are narrow jets of particles at relativistic speeds squirting off along the disk's axis.
However, accretion disks, jets, and orbiting objects are found not only around black holes, but also around other objects such as neutron stars; and the dynamics of bodies near these non-black hole objects is largely but not completely identical to the dynamics of bodies around black holes. Hence, for the most part, observations of accretion disks and orbital motions merely indicate that there is a compact object of a certain mass, and says very little about the nature of that object. The identification of an object as a black hole requires the further assumption that no other object (or bound system of objects) could be so massive and compact. Most astrophysicists accept that this is the case, since according to general relativity, any concentration of matter of sufficient density must necessarily collapse into a black hole.
One important observable difference between black holes and other compact massive objects is that any infalling matter will eventually collide with the latter, at relativistic speeds, leading to irregular intense flares of X-rays and other hard radiation. Thus the lack of such flare-ups around a compact concentration of mass is evidence that the object is a black hole, with no surface onto which matter can be suddenly dumped.
Have we found them?
which is widely accepted to be a 10 solar mass black hole orbiting a blue giant star]]There is now a great deal of indirect astronomical observational evidence for black holes in two mass ranges:
- stellar mass black holes with masses of a typical star (4–15 times the mass of our Sun), and
- supermassive black holes with masses perhaps 1% that of a typical galaxy (This evidence comes not from seeing the black holes directly, but by observing the behavior of stars and other material near them.
Candidates to stellar-mass black holes were identified mainly by the presence of accretion disks of the right size and speed, without the irregular flare-ups that are expected from disks around other compact objects. Stellar-mass black holes may be involved in gamma ray bursters (GRBs), although observations of GRBs in association with supernovae have reduced the possibility of a link.
Candidates for more massive black holes were first provided by the active galactic nuclei and quasars, discovered by radioastronomers in the 1960s. The efficient conversion of mass into energy by friction in the accretion disk of a black hole seems to be the only explanation for the copious amounts of energy generated by such objects. Indeed the introduction of this theory in the 1970s removed a major objection to the belief that quasars were distant galaxies — namely, that no physical mechanism could generate that much energy.
From observations in the 1980s of motions of stars around the galactic center, it is now believed that such supermassive black holes exist in the center of most galaxies, including our own Milky Way. Sagittarius A* is now agreed to be the most plausible candidate for the location of a supermassive black hole at the center of the Milky Way galaxy.
The current picture is that all galaxies may have a supermassive black hole in their center, and that this black hole swallows gas and dust in the middle of the galaxies generating huge amounts of radiation — until all the nearby mass has been swallowed and the process shuts off. This picture also nicely explains why there are no nearby quasars. Though the details are still not clear, it seems that the growth of the black hole is intimately related to the growth of the spheroidal component — an elliptical galaxy, or the bulge of a spiral galaxy — in which it lives. Interestingly, there is no evidence for massive black holes in the center of globular clusters, suggesting that these are fundamentally different than galaxies.
The formation of micro black holes on Earth in particle accelerators have been tentatively reported, but not yet confirmed. So far there are no observed candidates for primordial black holes.
Mathematical physics
Black holes are predictions of Albert Einstein's theory of general relativity. In particular, they occur in the Schwarzschild metric, one of the earliest and simplest solutions to Einstein's equations, found by Karl Schwarzschild in 1915. This solution describes the curvature of spacetime in the vicinity of a static and spherically symmetric object, with the metric is
- ,
According to Schwarzschild's solution, a gravitating object will collapse into a black hole if its radius is smaller than a characteristic distance, known as the Schwarzschild radius. Below this radius, spacetime is so strongly curved that any light ray emitted in this region, regardless of the direction in which it is emitted, will travel towards the center of the system. Because relativity forbids anything from travelling faster than light, anything below the Schwarzschild radius – including the constituent particles of the gravitating object – will collapse into the center. A gravitational singularity, a region of theoretically infinite density, forms at this point. Because not even light can escape from within the Schwarzschild radius, a classical black hole would truly appear black.
The Schwarzschild radius is given by in relativistic units as above, or
The mean density inside the Schwarzschild radius decreases as the mass of the black hole increases, so while an earth mass black hole would have a density of 2 × 10^{30} kg/m^{3}, a supermassive black hole of 10^{9} solar masses has a density of around 20 kg/m^{3}, less than water! The mean density is given by
More general black holes are also predicted by other solutions to Einstein's equations, such as the Kerr metric for a rotating black hole, which possesses a ring singularity, and the Reissner-Nordstrøm metric; for charged black holes.
Recent discoveries
In 2004 a cluster of black holes was detected, broadening our understanding of the frequency of black holes throughout out universe. It is now thought that scientists' inferences of how many black holes are in our universe were quite off until now. It is predicted due to these finds in 2004 that there are close to five fold the number of black holes that there were predicted to be before this discovery.In July, 2004 astronomers found a giant black hole, Q0906+6930, at the center of a distant galaxy in the Ursa Major constellation. The size and presumed age of the black hole has implications about the age of the universe [1].
Related topics
- Schwarzschild metric
- Schwarzschild radius = radius of a black hole
- compact stars
- timeline of black hole physics
- string theory
- white hole
- neutron star
- supermassive black hole
- Gravastar
External links
- Tufts University: Student Project (Great Kid's Section)
- Jilian’s Guide to Black Holes
- Supermassive Black Holes
- Schwarzschild Geometry
- FAQ on black holes
Further reading
- Thorne, Kip S. (1995). Black holes and time warps
- Wald, Robert M. (1992). Space, time, and gravity: the theory of the big bang and black holes
- Chandrasekhar, Subrahmanyan (1998). The Mathematical Theory of Black Holes
- Hawking, Stephen (1988). A Brief History of Time - And later editions. ISBN 0553380168