Phys. Rev. D 23, 287–298 (1981)Universal upper bound on the entropy-to-energy ratio for bounded systemsReceived 7 July 1980; revised 25 August 1980; published in the issue dated 15 January 1981 We present evidence for the existence of a universal upper bound of magnitude 2πR/ℏc to the entropy-to-energy ratio S/E of an arbitrary system of effective radius R. For systems with negligible self-gravity, the bound follows from application of the second law of thermodynamics to a gedanken experiment involving a black hole. Direct statistical arguments are also discussed. A microcanonical approach of Gibbons illustrates for simple systems (gravitating and not) the reason behind the bound, and the connection of R with the longest dimension of the system. A more general approach establishes the bound for a relativistic field system contained in a cavity of arbitrary shape, or in a closed universe. Black holes also comply with the bound; in fact they actually attain it. Thus, as long suspected, black holes have the maximum entropy for given mass and size which is allowed by quantum theory and general relativity. © 1981 The American Physical Society URL:
http://link.aps.org/doi/10.1103/PhysRevD.23.287
DOI:
10.1103/PhysRevD.23.287
PACS:
See AlsoComment: S. D. Unwin, Possible violations of the entropy-to-energy-ratio bound, Phys. Rev. D 26, 944 (1982). Comment: Don N. Page, Comment on a universal upper bound on the entropy-to-energy ratio for bounded systems, Phys. Rev. D 26, 947 (1982). Comment: Jacob D. Bekenstein, Specific entropy and the sign of the energy, Phys. Rev. D 26, 950 (1982). Comment: P. F. González-Díaz, Bounds on the entropy, Phys. Rev. D 27, 3042 (1983). |
