- Schwarzschild radius
The Schwarzschild radius (sometimes historically referred to as the gravitational radius) is a characteristic
radius associated with everymass . It is the radius for a given mass where, if that mass could be compressed to fit within that radius, no known force or degeneracy pressure could stop it from continuing to collapse into agravitational singularity . The term is used inphysics andastronomy , especially in the theory ofgravitation ,general relativity .In 1916,
Karl Schwarzschild obtained an exact solution [K. Schwarzschild, "Uber das Gravitationsfeld eines Massenpunktes nach der Einsteinschen Theorie", "Sitzungsberichte der Deutschen Akademie der Wissenschaften zu Berlin, Klasse fur Mathematik, Physik, und Technik" (1916) pp 189.] [K. Schwarzschild, "Uber das Gravitationsfeld einer Kugel aus inkompressibler Flussigkeit nach der Einsteinschen Theorie", "Sitzungsberichte der Deutschen Akademie der Wissenschaften zu Berlin, Klasse fur Mathematik, Physik, und Technik" (1916) pp 424.] toEinstein's field equation s for the gravitational field outside a non-rotating, spherically symmetric body (seeSchwarzschild metric ). The solution contained a term of the form 1/(2M-r); the value of r making this term singular has come to be known as the "Schwarzschild radius". The physical significance of this singularity, and whether this singularity could ever occur in nature, was debated for many decades; a general acceptance of the possibility of ablack hole did not occur until the second half of the 20th century.The Schwarzschild radius of an object is proportional to the mass. Accordingly, the
Sun has a Schwarzschild radius of approximately 3 km, while theEarth 's is only about 9 mm, the size of apeanut .An object smaller than its Schwarzschild radius is called a
black hole . The surface at the Schwarzschild radius acts as anevent horizon in a non-rotating body. (Arotating black hole operates slightly differently.) Neither light nor particles can escape through this surface from the region inside, hence the name "black hole". The Schwarzschild radius of the (currently hypothesized)Supermassive black hole at ourGalactic Center would be approximately 7.8 million km. The Schwarzschild radius of a sphere with a uniform density equal to thecritical density is equal to the radius of thevisible universe . [F. Melia, "The Edge of Infinity: Supermassive Black Holes in the Universe," Cambridge UniversityPress (2003) pp 124.]Formula for the Schwarzschild radius
The Schwarzschild radius is proportional to the mass, with a proportionality constant involving the
gravitational constant and the speed of light.The formula for the Schwarzschild radius can be found by setting theescape velocity to the speed of light, and is:
r_s = frac{2Gm}{c^2},where
: r_s is the Schwarzschild radius,
: G is the
gravitational constant ,: m is the mass of the gravitating object, and
: c is the
speed of light .For a solar mass black hole, the Schwarzschild radius is thus 2.96 km, and the Schwarzschild radius of any other black hole can then be found by:
r_s = 2.96 frac{M}{M_{odot km.This can be extended to show that an object of any density can be large enough to fall within its own Schwarzschild radius,:
V_s propto ho^{-1.5}.where: V_s is the volume of the object, and
: ho is its density.
Note that although the result is correct, general relativity must be used to properly derive the Schwarzschild radius. It is only a coincidence that
Newtonian physics produces the same result.Classification by Schwarzschild radius
upermassive black hole
If one accumulates matter of normal density (1000 kg/m³, for example, the density of water) up to about 150,000,000 times the mass of the Sun, such an accumulation will fall inside its own Schwarzschild radius and thus it would be a
supermassive black hole of 150,000,000 solar masses. (Supermassive black holes up to 18 billion solar masses have been observed [cite news
last = Bryner
first = Jenna
coauthors =
title = Colossal Black Hole Shatters the Scales
work =
pages =
language =
publisher = SPACE.COM
date = January 9, 2008
url = http://www.space.com/scienceastronomy/080109-aas-massive-black-holes.html
accessdate = 2008-04-02] .) The supermassive black hole in the center of our galaxy (3.7 million solar masses) constitutes observationally the most convincing evidence for the existence of black holes in general.It is thought that large black holes like these don't form directly in one collapse of a cluster of stars.Instead they may start as a stellar-sized black hole and grow larger by the accretion of matter and other black holes. The larger the mass of a galaxy, the larger is the mass of the supermassive black hole in its center.tellar black hole
If one accumulates matter at
nuclear density (the density of the nucleus of an atom, about 1018 kg/m³;neutron star s also reach this density), such an accumulation would fall within its own Schwarzschild radius at about 3 solar masses and thus would be astellar black hole .Primordial black hole
Conversely, a small mass has an extremely small Schwarzschild radius. A mass similar to Mount Everest has a Schwarzschild radius smaller than a
nanometre . Its average density at that size would be so high that no known mechanism could form such extremely compact objects. Such black holes might possibly be formed in an early stage of the evolution of the universe, just after theBig Bang , when densities were extremely high. Therefore these hypothetical baby black holes are calledprimordial black hole s.History
The significance of the singularity at 2M=r was first raised by
Jacques Hadamard , who, during a conference in Paris in 1922, asked what might happen if a physical system could ever obtain this singularity.Albert Einstein insisted that it could not, pointing out the dire consequences for the universe, and jokingly referred to the singularity as the "Hadamard disaster". [Hamed Moradi, " [http://www.maths.monash.edu.au/~hmoradi/Honours_Essay_2004.pdf An Early History of Black Holes] ", (2004) Monash University]Schwarzschild's original model of a star assumed an incompressible fluid; Einstein pointed out that this was an unreasonable assumption, as sound waves would propagate at infinite speed. In his own work, Einstein reconsidered a model of a star where the components of the star were orbiting masses, and showed that the orbital velocities would exceed the speed of light at the Schwarzschild radius. In 1939, he used this to argue that no such thing can happen, and so the singularity could not occur in nature. [A. Einstein, "On a Stationary System with Spherical Symmetry Consisting of Many Gravitating Masses", "Annals of Mathematics", (1939)] The same year,
Robert Oppenheimer andHartland Snyder considered a model of a dust cloud, where the dust particles of the cloud were moving radially, towards a single point, and showed that the dust particles could reach the singularity in finiteproper time . After passing the limit, Oppenheimer and Snyder noted thatlight cone s were directed inwards, and that no signal could escape outside. [J.R. Oppenheimer, H. Snyder, "On Continued Gravitational Contraction", "Physical Review" 56 (1939) p455.]ee also
*
black hole , a general survey
*Chandrasekhar limit , a second requirement for black hole formationClassification of black holes by type:
*Schwarzschild or static black hole
*rotating or Kerr black hole
*charged black hole or Newman black hole and Kerr-Newman black holeA classification of black holes by mass:
*micro black hole and extra-dimensional black hole
*primordial black hole , a hypothetical leftover of the Big Bang
*stellar black hole , which could either be a static black hole or a rotating black hole
*supermassive black hole , which could also either be a static black hole or a rotating black hole
*visible universe , if its density is thecritical density References
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