General Relativity: An Introduction for Physicists · Problem 15.20

Cosmological models — Hobson, Efstathiou & Lasenby

Physics · flat-radiation-only-friedmann-results

Problem

For the spatially flat, radiation-only, Friedmann model, prove the following useful results: a(t)=(tt0)1/2,H(t)=12t=H0(1+z)2,q0=1,ρr(t)=332πGt2.a(t) = \left(\frac{t}{t_0}\right)^{1/2}, \qquad H(t) = \frac{1}{2t} = H_0(1+z)^2, \qquad q_0 = 1, \qquad \rho_r(t) = \frac{3}{32\pi G t^2}.

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