paper

Thermal instability in the collisionally cooled gas

arXiv:1110.3644 · doi:10.1111/j.1365-2966.2011.20017.x

Abstract

We have presented the non-equilibrium (time-dependent) cooling rate and ionization state calculations for a gas behind shock waves with km s ( K). Such shock waves do not lead to the radiative precursor formation, i.e. the thermal evolution of a gas behind the shock waves are controlled by collisions only. We have found that the cooling rate in a gas behind the shock waves with km s ( K) differs considerably from the cooling rate for a gas cooled from K. It is well-known that a gas cooled from K is thermally unstable for isobaric and isochoric perturbations at $T \simgt 2\times 10^4$ K. We have studied the thermal instability in a collisionally controlled gas for shock waves with km s. We have found that the temperature range, where the postshock gas is thermally unstable, is significantly modified and depends on both gas metallicity and ionic composition of a gas before shock wave. For $Z \simgt 0.1Z_\odot$ the temperature range, where the thermal instability criterion for isochoric perturbations is not fulfilled, widens in comparison with that for a gas cooled from K, while that for isobaric perturbations remains almost without a change. For a gas behind shock waves with $v \simlt 65$ km s ($T_s \simlt 10^5$ K) is thermally stable to isochoric perturbations during full its evolution. We have shown that the transition from isobaric to isochoric cooling for a gas with $Z \simgt 0.1Z_\odot$ behind shock waves with K proceeds at lower column density layer behind a shock wave than that for a gas cooled from K. (abridged)

8 pages, 10 figures, accepted to MNRAS

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