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MASS LOADING AND COLLIMATION OF GALACTIC SUPERWINDS

机译:银河系超风的质量载荷和聚集

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We attempt to constrain (1) the site and amount of mass loading and (2) the collimator geometry for a galactic superwind observed in the starburst galaxy M82 by comparing predictions for the superwind pressure, temperature, and X-ray emission deduced from hydrodynamical simulations of the bipolar conical hot gas outflow with the observed central pressures and temperatures as well as X-ray properties of this galaxy. We conclude that the superwind in M82 must be a mass-loading wind: the total mass flux turns out to be 3-6 times higher than the mass deposition rate due to supernova ejecta only, thus implying that the resulting wind is "loaded" with the mass of evaporated gas clouds. Such a wind means that M82 must have ejected of ~10~8 solar mass gas into the halo over the lifetime of the starburst event, 2-3 x 10~7 yr. We have found a strong dependence of the wind X-ray emission properties on the amount of mass loading. We therefore have concluded that the wind X-ray emission provides a sensitive tool to probe ISM transformations associated with the supernova explosions in the center of starbursts similar to M82. Comparison of the predicted pressures and temperatures with the estimates inferred from observations for the center of M82 indicates that essentially all mass loading must be confined to a thin layer in the center of the starburst where supernova explosions occur rather than being distributed throughout the vertical extension of the disk. The simulation results have also shown that both a wide-angle, fanlike wind suggested by the optical data (the cone opening angle θ ~ 60°) and a much narrower, jetlike wind inferred from recent ROSAT data (θ = 22°) appear to be compatible with the observed X-ray constraints. However, the two cases imply quite different geometries for the central cavity where wind collimation occurs. The collimator must be wide (r ~ 500 pc) if the wind above the central gaseous disk has a wide cone opening angle, such as suggested by the optical data, θ ≈ 60°. For a jetlike wind of the type inferred recently from ROSAT data (θ = 22°), the collimator radius at the base of the wind must be close to that of the starburst region, r ~ 150 pc. For the X-ray properties to be compatible with those observed in M82, it is essential that the outflow is strongly collimated over the central ~ 1.5 kpc but becomes much less collimated in the halo. This model predicts an outward softening of the X-ray flux such that the effective temperature of the X-ray gas in the outer part of the emitting region is a factor of ~2 smaller than the temperature within the central ~1.5 kpc.
机译:我们试图通过比较由水动力模拟得出的超风压力,温度和X射线发射的预测,来限制(1)在大爆炸星系M82中观测到的银河超风的位置和数量,以及(2)准直仪的几何形状。观测到的中心压力和温度以及该星系的X射线特性,显示了双极锥形热气体流出量。我们得出的结论是,M82中的超风必须是质量加载风:总质量通量仅是由于超新星喷射而产生的质量沉积速率的3-6倍,因此这意味着产生的风将被“加载”蒸发的气体云团。这样的风意味着在星爆事件的整个寿命(2-3 x 10〜7年)内,M82必须向大气环中喷射出约10〜8个太阳质量气体。我们已经发现,风X射线发射特性对质量负载量的依赖性很大。因此,我们得出的结论是,风X射线辐射提供了一种灵敏的工具,可用来探测与M82类似的星暴中心超新星爆炸相关的ISM转换。将预测的压力和温度与从M82中心的观测值推断出的估计值进行比较表明,基本上所有的质量载荷都必须限制在发生超新星爆炸的爆炸形星团中心的薄层中,而不是分布在整个M82的垂直延伸范围内。磁盘。仿真结果还表明,光学数据所建议的广角扇状风(圆锥张开角θ〜60°)和从最新的ROSAT数据(θ= 22°)推断出的窄射流状风都出现了。与观察到的X射线约束兼容。但是,这两种情况表明发生风准直的中心腔的几何形状完全不同。如果中心气态圆盘上方的风具有较大的锥度开度角(如光学数据θ≈60°所示),则准直仪必须较宽(r〜500 pc)。对于最近从ROSAT数据推断出的类喷气风(θ= 22°),在风底的准直仪半径必须接近星爆区域的准直仪半径,r〜150 pc。为了使X射线特性与M82中观察到的特性兼容,必须在中心〜1.5 kpc处使出射流严格准直,但在光环中变得不那么准直。该模型预测了X射线通量的向外软化,以使发射区域外部X射线气体的有效温度比中心〜1.5 kpc内的温度小约2倍。

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