Fig. 2

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Temperature profiles in the dusty radiative shock test at t = 0.054t0 = 3.75 × 104 sec, for a variety of stopping times. For ts = 10−1, the gas temperature is that of a standard hydrodynamic shock, with only weak losses to dust and radiation; for ts = 10−7, Td, and Tg have come into equilibrium, and they (along with wx and Tr) match the results of the two-temperature radiative shock tests in Sect. 4.1 of (Melon Fuksman et al. 2021). We note that the signed “reduced flux” of wx = Fx/Er is denoted as f in their work.
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