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Black-hole thermodynamics

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In physics, black-hole thermodynamics is the area of study that seeks to reconcile the laws of thermodynamics with the existence of black-hole event horizons. As the study of the statistical mechanics of black-body radiation led to the advent of the theory of quantum mechanics, the effort to understand the statistical mechanics of black holes has had a deep impact upon the understanding of quantum gravity, leading to the formulation of the holographic principle.[1]

An artist's depiction of two black holes merging, a process in which the laws of thermodynamics are upheld



The second law of thermodynamics requires that black holes have entropy. If black holes carried no entropy, it would be possible to violate the second law by throwing mass into the black hole. The increase of the entropy of the black hole more than compensates for the decrease of the entropy carried by the object that was swallowed.

Starting from theorems proved by Stephen Hawking, Jacob Bekenstein conjectured that the black-hole entropy was proportional to the area of its event horizon divided by the Planck area. In 1973 Bekenstein suggested   as the constant of proportionality, asserting that if the constant was not exactly this, it must be very close to it. The next year, in 1974, Hawking showed that black holes emit thermal Hawking radiation[2][3] corresponding to a certain temperature (Hawking temperature).[4][5] Using the thermodynamic relationship between energy, temperature and entropy, Hawking was able to confirm Bekenstein's conjecture and fix the constant of proportionality at  :[6]


where   is the area of the event horizon, calculated at  ,   is Boltzmann's constant, and   is the Planck length. This is often referred to as the Bekenstein–Hawking formula. The subscript BH either stands for "black hole" or "Bekenstein–Hawking". The black-hole entropy is proportional to the area of its event horizon  . The fact that the black-hole entropy is also the maximal entropy that can be obtained by the Bekenstein bound (wherein the Bekenstein bound becomes an equality) was the main observation that led to the holographic principle.[1]

Although Hawking's calculations gave further thermodynamic evidence for black-hole entropy, until 1995 no one was able to make a controlled calculation of black-hole entropy based on statistical mechanics, which associates entropy with a large number of microstates. In fact, so called "no-hair" theorems[7] appeared to suggest that black holes could have only a single microstate. The situation changed in 1995 when Andrew Strominger and Cumrun Vafa calculated [8] the right Bekenstein–Hawking entropy of a supersymmetric black hole in string theory, using methods based on D-branes and string duality. Their calculation was followed by many similar computations of entropy of large classes of other extremal and near-extremal black holes, and the result always agreed with the Bekenstein–Hawking formula. However, for the Schwarzschild black hole, viewed as the most far-from-extremal black hole, the relationship between micro- and macrostates is expected to be clarified from the string-theoretical viewpoint. Various studies are in progress, but this has not yet been elucidated.

In loop quantum gravity (LQG)[9] it is possible to associate a geometrical interpretation to the microstates: these are the quantum geometries of the horizon. LQG offers a geometric explanation of the finiteness of the entropy and of the proportionality of the area of the horizon.[10][11] It is possible to derive, from the covariant formulation of full quantum theory (Spinfoam) the correct relation between energy and area (1st law), the Unruh temperature and the distribution that yields Hawking entropy.[12] The calculation makes use of the notion of dynamical horizon and is done for non-extremal black holes. There seems to be also discussed the calculation of Bekenstein–Hawking entropy from the point of view of LQG.

The laws of black-hole mechanicsEdit

The four laws of black-hole mechanics are physical properties that black holes are believed to satisfy. The laws, analogous to the laws of thermodynamics, were discovered by Brandon Carter, Stephen Hawking, and James Bardeen.

Statement of the lawsEdit

The laws of black-hole mechanics are expressed in geometrized units

The zeroth lawEdit

The horizon has constant surface gravity for a stationary black hole.

The first lawEdit

For perturbations of stationary black holes, the change of energy is related to change of area, angular momentum, and electric charge by


where   is the energy,   is the surface gravity,   is the horizon area,   is the angular velocity,   is the angular momentum,   is the electrostatic potential and   is the electric charge.

The second lawEdit

The horizon area is, assuming the weak energy condition, a non-decreasing function of time:


This "law" was superseded by Hawking's discovery that black holes radiate, which causes both the black hole's mass and the area of its horizon to decrease over time.

The third lawEdit

It is not possible to form a black hole with vanishing surface gravity.   is not possible to achieve.

Discussion of the lawsEdit

The zeroth lawEdit

The zeroth law is analogous to the zeroth law of thermodynamics, which states that the temperature is constant throughout a body in thermal equilibrium. It suggests that the surface gravity is analogous to temperature. T constant for thermal equilibrium for a normal system is analogous to   constant over the horizon of a stationary black hole.

The first lawEdit

The left side, dE, is the change in energy (proportional to mass). Although the first term does not have an immediately obvious physical interpretation, the second and third terms on the right side represent changes in energy due to rotation and electromagnetism. Analogously, the first law of thermodynamics is a statement of energy conservation, which contains on its right side the term T dS.

The second lawEdit

The second law is the statement of Hawking's area theorem. Analogously, the second law of thermodynamics states that the change in entropy in an isolated system will be greater than or equal to 0 for a spontaneous process, suggesting a link between entropy and the area of a black-hole horizon. However, this version violates the second law of thermodynamics by matter losing (its) entropy as it falls in, giving a decrease in entropy. However, generalizing the second law as the sum of black-hole entropy and outside entropy, shows that the second law of thermodynamics is not violated in a system including the universe beyond the horizon.

The third lawEdit

Extremal black holes[13] have vanishing surface gravity. Stating that   cannot go to zero is analogous to the third law of thermodynamics, which states that the entropy of a system at absolute zero is a well defined constant. This is because a system at zero temperature exists in its ground state. Furthermore, ΔS will reach zero at zero temperature, but S itself will also reach zero, at least for perfect crystalline substances. No experimentally verified violations of the laws of thermodynamics are known.

Interpretation of the lawsEdit

The four laws of black-hole mechanics suggest that one should identify the surface gravity of a black hole with temperature and the area of the event horizon with entropy, at least up to some multiplicative constants. If one only considers black holes classically, then they have zero temperature and, by the no-hair theorem,[7] zero entropy, and the laws of black-hole mechanics remain an analogy. However, when quantum-mechanical effects are taken into account, one finds that black holes emit thermal radiation (Hawking radiation) at a temperature


From the first law of black-hole mechanics, this determines the multiplicative constant of the Bekenstein–Hawking entropy, which is


Beyond black holesEdit

Hawking and Page have shown that black-hole thermodynamics is more general than black holes—that cosmological event horizons also have an entropy and temperature.

More fundamentally, 't Hooft and Susskind used the laws of black-hole thermodynamics to argue for a general holographic principle of nature, which asserts that consistent theories of gravity and quantum mechanics must be lower-dimensional. Though not yet fully understood in general, the holographic principle is central to theories like the AdS/CFT correspondence.[14]

There are also connections between black-hole entropy and fluid surface tension.[15]

See alsoEdit


  1. ^ a b Bousso, Raphael (2002). "The Holographic Principle". Reviews of Modern Physics. 74 (3): 825–874. arXiv:hep-th/0203101 . Bibcode:2002RvMP...74..825B. doi:10.1103/RevModPhys.74.825. 
  2. ^ "First Observation of Hawking Radiation" from the Technology Review.
  3. ^ Matson, John (Oct 1, 2010). "Artificial event horizon emits laboratory analogue to theoretical black hole radiation". Sci. Am. 
  4. ^ Charlie Rose: A conversation with Dr. Stephen Hawking & Lucy Hawking Archived March 29, 2013, at the Wayback Machine.
  5. ^ A Brief History of Time, Stephen Hawking, Bantam Books, 1988.
  6. ^ Majumdar, Parthasarathi (1999). "Black Hole Entropy and Quantum Gravity". Indian J. Phys. 73.21: 147. arXiv:gr-qc/9807045 . Bibcode:1999InJPB..73..147M. 
  7. ^ a b Bhattacharya, Sourav (2007). "Black-Hole No-Hair Theorems for a Positive Cosmological Constant". Physical Review Letters. 99 (20): 201101. arXiv:gr-qc/0702006 . Bibcode:2007PhRvL..99t1101B. doi:10.1103/PhysRevLett.99.201101. PMID 18233129. 
  8. ^ Strominger, A.; Vafa, C. (1996). "Microscopic origin of the Bekenstein-Hawking entropy". Physics Letters B. 379: 99. arXiv:hep-th/9601029 . Bibcode:1996PhLB..379...99S. doi:10.1016/0370-2693(96)00345-0. 
  9. ^ See List of loop quantum gravity researchers.
  10. ^ Rovelli, Carlo (1996). "Black Hole Entropy from Loop Quantum Gravity". Physical Review Letters. 77 (16): 3288–3291. arXiv:gr-qc/9603063 . Bibcode:1996PhRvL..77.3288R. doi:10.1103/PhysRevLett.77.3288. 
  11. ^ Ashtekar, Abhay; Baez, John; Corichi, Alejandro; Krasnov, Kirill (1998). "Quantum Geometry and Black Hole Entropy". Physical Review Letters. 80 (5): 904–907. arXiv:gr-qc/9710007 . Bibcode:1998PhRvL..80..904A. doi:10.1103/PhysRevLett.80.904. 
  12. ^ Bianchi, Eugenio (2012). "Entropy of Non-Extremal Black Holes from Loop Gravity". arXiv:1204.5122  [gr-qc]. 
  13. ^ Kallosh, Renata (1992). "Supersymmetry as a cosmic censor". Physical Review D. 46 (12): 5278–5302. arXiv:hep-th/9205027 . Bibcode:1992PhRvD..46.5278K. doi:10.1103/PhysRevD.46.5278. 
  14. ^ For an authoritative review, see Ofer Aharony; Steven S. Gubser; Juan Maldacena; Hirosi Ooguri; Yaron Oz (2000). "Large N field theories, string theory and gravity". Physics Reports. 323 (3–4): 183–386. arXiv:hep-th/9905111 . Bibcode:1999PhR...323..183A. doi:10.1016/S0370-1573(99)00083-6. 
  15. ^ Callaway, D. (1996). "Surface tension, hydrophobicity, and black holes: The entropic connection". Physical Review E. 53 (4): 3738–3744. arXiv:cond-mat/9601111 . Bibcode:1996PhRvE..53.3738C. doi:10.1103/PhysRevE.53.3738. PMID 9964684. 


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