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The Glimm scheme for perfect fluids on plane-symmetric Gowdy spacetimes

A P Barnes1, P G Lefloch2, B G Schmidt3 and J M Stewart1

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We propose a new, augmented formulation of the coupled Euler–Einstein equations for perfect fluids on plane-symmetric Gowdy spacetimes. The unknowns of the augmented system are the density and velocity of the fluid and the first- and second-order spacetime derivatives of the metric. We solve the Riemann problem for the augmented system, allowing propagating discontinuities in both the fluid variables and the first- and second-order derivatives of the geometry coefficients. Our main result, based on Glimm's random choice scheme, is the existence of solutions with bounded total variation of the Euler–Einstein equations, up to the first time where a blow-up singularity (unbounded first-order derivatives of the geometry coefficients) occurs. We demonstrate the relevance of the augmented system for numerical relativity. We also consider general vacuum spacetimes and solve a Riemann problem, by relying on a theorem by Rendall on the characteristic value problem for the Einstein equations.


PACS

04.20.Cv Fundamental problems and general formalism

04.25.D- Numerical relativity

04.20.Ex Initial value problem, existence and uniqueness of solutions

47.75.+f Relativistic fluid dynamics

MSC

83C05 Einstein's equations (general structure, canonical formalism, Cauchy problems)

Subjects

Fluid dynamics

Gravitation and cosmology

Dates

Issue 22 (21 November 2004)

Received 31 August 2004

Published 20 October 2004



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