“…where ρ is the plasma mass density, is the fluid velocity, k R and k P are, respectively, the Rosseland and Planck mean opacities, c the speed of light, F the comoving-frame radiation flux, E the plasma internal energy density, E the comoving-frame radiation energy, k B the Boltzmann constant, T the plasma temperature, µ the mean particle weight (assuming solar abundances), m H the hydrogen mass, λ the flux-limiter (Minerbo 1978), and γ = 5/3 the ratio of specific heats. In a companion paper (Colombo et al 2019a; in the following Paper I), we discuss the assumptions and the limits of these equations. Since we are interested in evaluating the effects of irradiation from the post-shock accreting material on the pre-shock accretion column, we neglect the radiation effects (both radiative losses and absorption of radiation by matter) in the pre-shock chromosphere (i.e., k P = k R = 0 and L = 0 in Eqs.…”