Remark concerning spherically symmetric nonstatic solutions to the Einstein equations in the comoving frame

Physics

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All nonstatic spherically symmetric fluid solutions to the Einstein equations in the comoving frame ds^2 = e^{λ (r,t)} dr^2 + e^{μ (r,t)} dΩ ^2 - e^{v(r,t)} dt^2 are found subject to the conditions: (i)dot λ = Adot μ,A = const, (ii) λ,μ, andν are separable functions ofr andt, (iii) the heat flux vanishes, and (iv) the coefficient of shear viscosity vanishes. There are but two classes of solutions: (i)A= 1, in which case the metric reduces to the Robertson-Walker form, and (ii)A=0, in which case there are four solutions, all with nonvanishing acceleration, expansion, and shear. WithA=0, the solutions are either singular at the origin or degenerate into spaces of constant curvature.

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