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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.磁化的介质

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Observations have suggested substantial departures from pressure equilibrium in the interstellar medium (ISM) in the plane of the Galaxy, even on scales under 50 pc. Nevertheless, multiphase models of the ISM assume at least locally isobaric gas. The pressure then determines the density reached by gas cooling to stable thermal equilibrium. We use numerical models of the magnetized ISM to examine the consequences of supernova driving for interstellar pressures. In this paper we examine a (200 pc)~3 periodic domain threaded by magnetic fields. Individual parcels of gas at different pressures reach widely varying points on the thermal equilibrium curve: no unique set of phases is found but rather a dynamically determined continuum of densities and temperatures. A substantial fraction of the gas remains entirely out of thermal equilibrium. Our results appear consistent with observations of interstellar pressures. They also suggest that the high pressures observed in molecular clouds may be due to ram pressures in addition to gravitational forces. Much of the gas in our model lies far from equipartition between thermal and magnetic pressures, with ratios ranging from 0.1 to 10~4 and ratios of uniform to fluctuating magnetic field of 0.5-1. Our models show broad pressure probability distribution functions with log-normal functional forms produced by both shocks and rarefaction waves rather than power-law distributions produced by isolated supernova remnants. The width of the distribution can be described quantitatively by a formula derived from the work of Padoan, Nordlund, & Jones.
机译:观察结果表明,即使在50 pc以下的尺度上,星际平面中星际介质(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,压力决定了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的数值模型来检查超新星驱动对星际压力的影响。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。很大一部分气体仍完全不处于热平衡状态。我们的结果似乎与星际压力的观测结果一致。他们还建议,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,均匀磁场和波动磁场的比率为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和Jones的工作中得出的公式进行定量描述。

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