Abstract

Different from Milky Way-like galaxies, discs of gas-rich galaxies are clumpy. It is believed that the clumps form because of gravitational instability. However, a necessary condition for gravitational instability to develop is that the disc must dissipate its kinetic energy effectively, this energy dissipation (also called cooling) is not well understood. We propose that collisions (coagulation) between molecular clouds dissipate the kinetic energy of the discs, which leads to a dynamical cooling. The effectiveness of this dynamical cooling is quantified by the dissipation parameter D, which is the ratio between the free-fall time |$t_{\rm ff}\approx 1/ \sqrt{G \rho _{\rm {\rm disc}}}$| and the cooling time determined by the cloud collision process tcool. This ratio is related to the ratio between the mean surface density of the disc Σdisc and the mean surface density of molecular clouds in the disc Σcloud. When D < 1/3 (which roughly corresponds to |$\Sigma _{\rm {\rm disc}} < 1/3 \Sigma _{\rm cloud}$|⁠), cloud collision cooling is inefficient, and fragmentation is suppressed. When D > 1/3 (which roughly corresponds to Σdisc > 1/3Σcloud), cloud–cloud collisions lead to a rapid cooling through which clumps form. On smaller scales, cloud–cloud collisions can drive molecular cloud turbulence. This dynamical cooling process can be taken into account in numerical simulations as a sub-grid model to simulate the global evolution of disc galaxies.

Highlights

  • Star formation occurs in the cold phase of the galactic interstellar medium (ISM), which exhibits diverse morphologies in different galaxies

  • We argue that there is another consequence of cloud-cloud collisions, namely that these collisions should lead to a dissipation of kinetic energy in the disc, where the disc kinetic energy is converted into molecular cloud turbulence through these collisions

  • We study the evolution of galactic discs, and aim to understand the formation mechanism of the kpc-sized giant clumps commonly observed in gas-rich discs

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Summary

INTRODUCTION

Star formation occurs in the cold phase of the galactic interstellar medium (ISM), which exhibits diverse morphologies in different galaxies. The kinetic energy contained in these motions cannot be reduced with the radiative cooling, and additional dynamical cooling channels are needed Another set of models are based on the picture of galactic disc turbulence (Wada et al 2002; Elmegreen & Burkert 2010; Klessen & Hennebelle 2010; Elmegreen 2011; Forbes et al 2014). The previous studies on cloud-cloud collisions in galaxies (Kwan & Valdes 1983; Marochnik et al 1983; Tomisaka 1986; Tan 2000; Vollmer & Beckert 2002; Dobbs 2008) mainly considered the evolution of clouds in fixed galactic potentials and focused on properties of the clouds In their restricted settings, clouds are usually not allowed to back-react on the disc dynamics. When the collision rate is high, clumps form as a result of the collective motion of the molecular clouds included by cloud collision cooling

THE MODEL
General picture
Disc cooling through cloud-cloud collisions
Impact of cooling on disc fragmentation
Surface densities of clouds
Condition of clump formation
Kinetic energy budged and driving of molecular cloud turbulence
CONNECTION TO OBSERVATIONS
CONCLUSIONS
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