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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 35 (1994), S. 4809-4831 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: This article is a discussion of how it is possible to do perturbation theory for the Einstein–Boltzmann system about a dust solution. Explicitly expressed, the background Robertson–Walker universe model and one-parameter families of exact solutions are applied to the Einstein–Boltzmann system to obtain a closed-form solution of the equations governing linearized perturbations at late times, when the nonzero pressure of the gas of massive particles may be regarded as being significantly smaller than the energy density. After splitting the distribution function into two structurally different parts, the analysis given here provides a means of deriving the equations of linear hydrodynamics. In fact, due to the specific properties of the background chosen, one can prove that the evolution of suitably defined hydrodynamic variables is exactly decoupled from the evolution of the phase-space function satisfying the linearized Boltzmann equation. For simplicity, the workings of the method are illustrated by assuming that the perturbed metric is also of the Robertson–Walker form. A detailed treatment of the effect of inhomogeneities in an almost-Robertson–Walker universe model will be the subject of the last article in this series.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 35 (1994), S. 5885-5907 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: This is the second in a pair of articles, the overall objective of which is to describe within the framework of the Einstein–Boltzmann system a self-consistent perturbation method which leads to a tractable set of integrodifferential equations for the rate of change of the metric and the distribution function. The main purpose here is to prove that, for cases where the pressure of the gas of massive particles vanishes in the background, the treatment of the Einstein–Boltzmann system by means of a suitable perturbation method automatically produces a complete scheme of hydrodynamics, consisting of a closed set of partial differential equations for the evaluation of the mean velocity, the mass density, the temperature or the pressure, and the metric. The growing hydrodynamic modes are systematically derived for an almost-Robertson–Walker universe model, and the calculations are proposed without making any restrictions on the form of the perturbed metric. To summarize, the present article suggests a scheme of hydrodynamics for the late stages of cosmic expansion and calls attention to the support and interpretation given by the general-relativistic kinetic theory of monatomic gases to this scheme. Comparison with the predictions of the Eckart and/or Landau–Lifshitz theories of dissipative fluids is also briefly presented.
    Type of Medium: Electronic Resource
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