1982
DOI: 10.1093/mnras/201.4.833
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The dynamical destruction of shocked gas clouds

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Cited by 80 publications
(41 citation statements)
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“…For strong shocks, the cloud crushing time depends on the density contrast between the cloud and the ambient medium, the size of the cloud, and the speed of the shock. Earlier under-resolved numerical work came to similar conclusions (Nittmann et al 1982;Bedogni & Woodward 1990). These studies found that shocked clouds travel ∼8 cloud radii before mixing with the ambient medium as a result of hydrodynamic instabilities.…”
Section: Introductionsupporting
confidence: 69%
“…For strong shocks, the cloud crushing time depends on the density contrast between the cloud and the ambient medium, the size of the cloud, and the speed of the shock. Earlier under-resolved numerical work came to similar conclusions (Nittmann et al 1982;Bedogni & Woodward 1990). These studies found that shocked clouds travel ∼8 cloud radii before mixing with the ambient medium as a result of hydrodynamic instabilities.…”
Section: Introductionsupporting
confidence: 69%
“…In the most well known simulations ( Nittmann et al 1982;KMC;Mac Low et al 1994;Nakamura et al 2006), it is assumed that a low-density molecular cloud with no selfgravity or magnetic fields is exposed to a steady shock. The shock collides with the cloud, producing a reverse shock that develops into a bow shock; a shock propagates through the cloud, passing through it in a ''cloud crushing'' time t cc .…”
Section: This Raises the Question If Our Resolution Is Not As Good Amentioning
confidence: 99%
“…When an adiabatic cloud is impacted, it passes through four characteristic phases: compression, re-expansion, fragmentation and mixing with the ISM (see, e.g., Nittmann et al 1982;McKee 1988;Klein et al 1994). Its gas is initially compressed by an internal forward shock wave that crosses the cloud in a time t crush ∼ t SC q 0.5 , where q = ρ c /ρ sh is the ratio between the density of the cloud and the SSSF.…”
Section: Setmentioning
confidence: 99%