Fundamental thermodynamical equation of a self-gravitating system
Erik A. Martinez (Center for Gravitational Physics, Geometry, Penn, State, USA)

TL;DR
This paper explores the unique thermodynamical relations of self-gravitating systems, including models like shells and black holes, analyzing stability, entropy, and the influence of gravity on thermodynamic laws.
Contribution
It develops a formal thermodynamic framework for self-gravitating systems, connecting Einstein equations with thermodynamics and analyzing entropy and stability during collapse.
Findings
Entropy growth during shell collapse matches black hole entropy under certain conditions
Thermodynamics of self-gravitating systems lacks a Gibbs-Duhem relation
Intrinsic stability depends on the thermal equation of state
Abstract
The features of the fundamental thermodynamical relation (expressing entropy as function of state variables) that arise from the self-gravitating character of a system are analyzed. The models studied include not only a spherically symmetric hot matter shell with constant particle number but also a black hole characterized by a general thermal equation of state. These examples illustrate the formal structure of thermodynamics developed by Callen as applied to a gravitational configuration as well as the phenomenological manner in which Einstein equations largely determine the thermodynamical equations of state. We consider in detail the thermodynamics and quasi-static collapse of a self-gravitating shell. This includes a discussion of intrinsic stability for a one-parameter family of thermal equations of state and the interpretation of the Bekenstein bound. The entropy growth associated…
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