Black hole entropy
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The proposal, made by Jacob Bekenstein in the early 1970s and given its coefficient by Hawking's 1974 temperature, that a black hole carries entropy proportional to the area of its horizon rather than to any volume. It resolved an apparent violation of the second law - throw a hot gas into a black hole and the entropy of the universe seems to fall - by giving the hole an entropy of its own that necessarily rises. The numbers are extreme: a solar-mass black hole carries an entropy some twenty orders of magnitude larger than the star that formed it, which is another way of saying that almost all the information about that star has become inaccessible. Because the quantity scales with area and not volume, it is the origin of the holographic principle, the suggestion that the degrees of freedom of a region can be accounted for on its boundary. String theory reproduced the exact coefficient for certain highly symmetric extremal black holes in 1996, which is regarded as a genuine success; the general case is not derived. Not a place on Earth.
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Timeline
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Connections · 3
- The event horizonconcerns
- Jacob Bekensteincreated_by
- Hawking radiationdepends_on
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Assembled from 34 blocks · 2 evidence · 27 related
- Story
- The proposal, made by Jacob Bekenstein in the early 1970s and given its coefficient by Hawking's 1974 temperature, that a black hole carries entropy proportional to the area of its horizon rather than to any volume. It resolved an apparent violation of the second law - throw a hot gas into a black hole and the entropy of the universe seems to fall - by giving the hole an entropy of its own that necessarily rises. The numbers are extreme: a solar-mass black hole carries an entropy some twenty orders of magnitude larger than the star that formed it, which is another way of saying that almost all the information about that star has become inaccessible. Because the quantity scales with area and not volume, it is the origin of the holographic principle, the suggestion that the degrees of freedom of a region can be accounted for on its boundary. String theory reproduced the exact coefficient for certain highly symmetric extremal black holes in 1996, which is regarded as a genuine success; the general case is not derived. Not a place on Earth.
- Knowledge
- The event horizon
- Hawking radiation
- Black hole entropy
- Jacob Bekenstein
- Connections
- The event horizon
- Jacob Bekenstein
- Hawking radiation
- Bekenstein assigns entropy to a black hole
- Hawking shows that black holes radiate
- Page states what unitarity requires of the radiation
- The Page curve is reproduced from within semiclassical gravity
- The Kerr solution and black hole spin
- Schwarzschild radius
- Black hole entropy
- Schwarzschild solves the field equations for a point mass
- Oppenheimer and Snyder compute continued gravitational contraction
- Penrose proves that collapse to a singularity is generic
- The term "black hole" enters use
- GW150914 - two black holes merge and the signal reaches Earth
- Black hole entropy
- Bekenstein assigns entropy to a black hole
- Stephen Hawking
- Black hole entropy
- The black hole information paradox
- Hawking shows that black holes radiate
- Hawking argues that information is destroyed
- The Page curve is reproduced from within semiclassical gravity
- Evidence
- Proposes that a black hole carries entropy proportional to the area of its horizon, in order to preserve the second law of thermodynamics. V55 VERIFICATION BASIS: not consulted in session; no research tool was available. Volume and page are from recall and must be checked.
- Derives thermal emission from a black hole horizon at a temperature inversely proportional to mass. V55 VERIFICATION BASIS: not consulted in session; no research tool was available. Volume and page are from recall of a canonical citation and must be checked. The fuller treatment appeared in Communications in Mathematical Physics in 1975 and is deliberately not cited by volume here.
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