Effective Pressure of the FRW Universe
arXiv:2507.17789 · doi:10.1016/j.aop.2025.170163
Abstract
In this paper, we study the effective pressure of the -dimensional FRW(Friedmann-Robertson-Walker) universe in Einstein gravity, Gauss-Bonnet gravity, and Lovelock gravity. The effective pressure is defined by , where is the effective energy and is the volume of the FRW universe inside the apparent horizon. The effective pressure in Einstein gravity is always negative and its absolute value decreases with the horizon radius . The effective pressure in Gauss-Bonnet gravity is different with the one in Einstein gravity only when . In this case, if , the effective pressure is always negative, but if , it is not always negative and has a minimum. The effective pressure in Lovelock gravity can have multiple zero-points and extreme points. The effective pressure in different dimensions has interesting relations. We also find that under certain condition, the effective pressure is equivalent with the `ordinary' pressure of the perfect fluid, and this condition do not depend on the specific choice of gravitational theories.
9 pages,2 figures
References in corpus (6)
- Thermodynamic Behavior of Friedmann Equation at Apparent Horizon of FRW Universe
- Unified First Law and Thermodynamics of Apparent Horizon in FRW Universe
- The minus sign in the first law of de Sitter horizons
- Phase Transitions and Critical Phenomena for the FRW Universe in an Effective Scalar-Tensor Theory
- Equation of State and Joule-Thomson Expansion for the FRW Universe in the Brane World Scenario
- Thermodynamics of the arbitrary dimensional FRW universe: Joule-Thomson expansion