Complementary role of the pressure in the black hole thermodynamics

Abstract

In black hole thermodynamics of certain models, the thermodynamic first law may contain the pressure term. The corresponding entropy follows the area law whereas the thermodynamic energy is not the same with the black hole mass. If the pressure can be decomposed into two parts and recombined with the original thermodynamic quantities, then the thermodynamic energy becomes the black hole mass and the entropy satisfying the area law turns out to be the corrected entropy called the Wald entropy, respectively.

arXiv commentv2. version to appear in PRD; 7 pages, references added

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• Horizon thermodynamics in fourth-order gravity
• Thermodynamics from field equations for black holes with multiple horizons