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MOLECULAR CLOUD EVOLUTION. Ⅰ. MOLECULAR CLOUD AND THIN COLD NEUTRAL MEDIUM SHEET FORMATION

机译:分子云的演变。 Ⅰ。分子云和薄冷中性板的形成

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We discuss molecular cloud formation by large-scale supersonic compressions in the diffuse warm neutral medium (WNM). Initially, a shocked layer forms, and within it, a thin cold layer. An analytical model and high-resolution one-dimensional simulations predict the thermodynamic conditions in the cold layer. After ~1 Myr of evolution, the layer has column density ~2.5 x 10~(19) cm~(-2), thickness ~0.03 pc, temperature ~25 K, and pressure ~6650 K cm~(-2). These conditions are strongly reminiscent of those recently reported by Heiles and coworkers for cold neutral medium sheets. In the one-dimensional simulations, the inflows into the sheets produce line profiles with a central line of width ~0.5 km s~(-1) and broad wings of width ~1 km s~(-1). Three-dimensional numerical simulations show that the cold layer develops turbulent motions and increases its thickness until it becomes a fully three-dimensional turbulent cloud. Fully developed turbulence arises on times ranging from ~7.5 Myr for inflow Mach number M_(1,r) = 2.4 to > 80 Myr for M_(1,r) = 1.03. These numbers should be considered upper limits. The highest density turbulent gas (HDG, n > 100 cm~(-3)) is always overpressured with respect to the mean WNM pressure by factors of 1.5-4, even though we do not include self-gravity. The intermediate-density gas (IDG, 10 < n/cm~(-3) < 100) has a significant pressure scatter that increases with M_(1,r), so that at M_(1,r) = 2.4 a significant fraction of the IDG is at a higher pressure than the HDG. Our results suggest that the turbulence and at least part of the excess pressure in molecular clouds can be generated by the compressive process that forms the clouds themselves and that thin CNM sheets may be formed transiently by this mechanism, when the compressions are only weakly supersonic.
机译:我们讨论了在弥散温暖的中性介质(WNM)中通过大规模超声压缩形成的分子云。最初,一个冲击层会在其内部形成一个薄的冷层。分析模型和高分辨率一维模拟可预测冷层的热力学条件。经过〜1 Myr演化后,该层的柱密度为〜2.5 x 10〜(19)cm〜(-2),厚度为〜0.03 pc,温度为〜25 K,压力为〜6650 K cm〜(-2)。这些条件使人想起了Heiles和他的同事最近针对冷中性纸张的报道。在一维模拟中,流入薄板的流水线产生的线轮廓的中心线宽约0.5 km s〜(-1),宽翼宽约1 km s〜(-1)。三维数值模拟表明,冷层会产生湍流运动并增加其厚度,直到它变成完全三维的湍流云为止。在流入马赫数M_(1,r)= 2.4的时间约为7.5 Myr到M_(1,r)= 1.03的> 80 Myr的时间范围内,会出现充分发展的湍流。这些数字应视为上限。即使不包括自重,最高密度的湍流气体(HDG,n> 100 cm〜(-3))也总是相对于平均WNM压力超压1.5-4倍。中密度气体(IDG,10

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