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The Distribution of Pressures in a Supernova-Driven Interstellar Medium. I. Magnetized Medium

机译:超新星驱动的星际介质中的压力分布。   I.磁化介质

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摘要

Observations have suggested substantial departures from pressure equilibriumin the interstellar medium (ISM) in the plane of the Galaxy, even on scalesunder 50 pc. Nevertheless, multi-phase models of the ISM assume at leastlocally isobaric gas. The pressure then determines the density reached by gascooling to stable thermal equilibrium. We use numerical models of themagnetized ISM to examine the consequences of supernova driving forinterstellar pressures. In this paper we examine a (200 pc)^3 periodic domainthreaded by magnetic fields. Individual parcels of gas at different pressuresreach widely varying points on the thermal equilibrium curve: no unique set ofphases is found, but rather a dynamically-determined continuum of densities andtemperatures. A substantial fraction of the gas remains entirely out of thermalequilibrium. Our results appear consistent with observations of interstellarpressures. They also suggest that the high pressures observed in molecularclouds may be due to ram pressures in addition to gravitational forces. Much ofthe gas in our model lies far from equipartition between thermal and magneticpressures, with ratios ranging from 0.1 to $10^4$ and ratios of uniform tofluctuating magnetic field of 0.5--1. Our models show broad pressureprobability distribution functions with log-normal functional forms produced byboth shocks and rarefaction waves, rather than power-law distributions producedby isolated supernova remnants. The width of the distribution can be describedquantitatively by a formula derived from the work of Padoan, Nordlund, & Jones(1997).
机译:观测结果表明,即使在50 pc以下的尺度下,星系平面中星际介质(ISM)中的压力平衡也有很大偏差。尽管如此,ISM的多相模型至少假设了局部等压气体。然后,压力确定通过气体冷却达到稳定的热平衡所达到的密度。我们使用磁化ISM的数值模型来检验超新星驱动星际压力的后果。在本文中,我们研究了一个由磁场穿过的(200 pc)^ 3周期域。在不同压力下的单个气体包裹到达热平衡曲线上的广泛变化的点:找不到唯一的相集,而是动态确定的密度和温度连续体。很大一部分气体完全没有热平衡。我们的结果似乎与星际压力的观测结果一致。他们还暗示,在分子云中观察到的高压可能是由于重力以外的冲压压力所致。我们模型中的大部分气体都远没有达到热压和磁压之间的均分,比率范围为0.1到$ 10 ^ 4 $,均匀波动磁场的比率为0.5--1。我们的模型显示了由压力和稀疏波产生的具有对数正态函数形式的宽压力概率分布函数,而不是由孤立的超新星残余产生的幂律分布。分布的宽度可以通过从Padoan,Nordlund,&Jones(1997)的工作中得出的公式定量地描述。

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