Introduction to Cosmology Ryden · Problem 5.5

Model Universes

Physics — Astrophysics · phantom-energy-big-rip

Problem

One speculation in cosmology is that the dark energy may take the form of ``phantom energy'' with an equation-of-state parameter w<−1w < -1. Suppose that the universe is spatially flat and contains matter with a density parameter Ωm,0\Omega_{m,0}, and phantom energy with a density parameter Ωp,0=1−Ωm,0\Omega_{p,0} = 1 - \Omega_{m,0} and equation-of-state parameter wp<−1w_p < -1. At what scale factor ampa_{mp} are the energy density of phantom energy and matter equal? Write down the Friedmann equation for this universe in the limit that a≫ampa \gg a_{mp}. Integrate the Friedmann equation to show that the scale factor aa goes to infinity at a finite cosmic time tript_{\rm rip}, given by the relation H0(trip−t0)≈23∣1+wp∣(1−Ωm,0)−1/2.(5.119)H_0(t_{\rm rip} - t_0) \approx \frac{2}{3|1+w_p|}(1 - \Omega_{m,0})^{-1/2}. \tag{5.119} This fate for the universe is called the ``Big Rip.'' Current observations of our own universe are consistent with H0=68H_0 = 68 km s−1^{-1} Mpc−1^{-1}, Ωm,0=0.3\Omega_{m,0} = 0.3, and wp=−1.1w_p = -1.1. If these numbers are correct, how long do we have remaining until the ``Big Rip''?

Related theory

Browse the problem library