2012/09/12 by Olivier Minazzoli, Tiberiu Harko · 1 citation
Physics and Astronomy · Mathematics · #gr-qc #astro-ph.CO #math-ph #math.MP
paper · pdf · doi:10.1103/physrevd.86.087502
published as Phys. Rev. D 86, 087502 (2012)
arxiv created 2012/09/12 · arxiv updated 2012/10/11
In this paper we give a simple proof that when the particle number is conserved, the Lagrangian of a barotropic perfect fluid is Lm=-ρ[c2 +∫ P(ρ)/ρ2 dρ], where ρ is the rest mass density and P(ρ) is the pressure. To prove this result nor additional fields neither Lagrange multipliers are needed. Besides, the result is applicable to a wide range of theories of gravitation. The only assumptions used in the derivation are: 1) the matter part of the Lagrangian does not depend on the derivatives of the metric, and 2) the particle number of the fluid is conserved (∇σ(ρuσ)=0).