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C. Cole, N. Demarais, Zhibo Yang, T. Snow, V. Bierbaum
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引用次数: 0

摘要

大量的研究探讨了热不稳定性在调节星际介质的冷云和热漫射介质之间的相变中的作用。研究热不稳定流中的湍流特性也引起了相当大的兴趣,特别强调分子云和恒星形成的可能性。在这项研究中,我们研究了另一种情况,其中这种不稳定性可能是重要的,即它对星际流中发电机作用的影响。我们考虑的设置是一个三维周期性立方体气体,初始磁场弱,受加热和冷却,其性质是这样的,热不稳定性在一定的温度范围内引起。发电机作用是通过对流场施加外力而建立的。通过将结果与具有完全相同净效应但没有热不稳定状态的冷却函数进行比较,我们发现如下。观察到非螺旋力的参考运行在雷诺数97以下不产生小尺度发电机作用。因此,我们预计在螺旋运行中产生的磁场纯粹是由于大型发电机机构的作用。在热稳定和不稳定运行之间,观察到大型发电机开始的临界雷诺数大约翻了一番,结论是热不稳定使大型发电机的作用更加困难。在热稳定的情况下,密度和磁场几乎完全不相关,而热不稳定的作用则产生了形式B∝ρ0.2的正相关。这种相关性是相当弱的,此外,它被观察到在最高密度的极限处被破坏。
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Numerous studies have investigated the role of thermal instability in regulating the phase transition between the cold cloudy and warm diffuse medium of the interstellar medium. Considerable interest has also been devoted to investigating the properties of turbulence in thermally unstable flows, with a special emphasis on molecular clouds and the possibility of star formation. In this study, we investigate another setting in which this instability may be important, namely its effect on dynamo action in interstellar flows. The setup we consider is a three-dimensional periodic cube of gas with an initially weak magnetic field, subject to heating and cooling, the properties of which are such that thermal instability is provoked in a certain temperature regime. Dynamo action is established through external forcing on the flow field. By comparing the results with a cooling function with exactly the same net effect but no thermally unstable regime, we find the following. Reference runs with non-helical forcing were observed to produce no small-scale dynamo action below the Reynolds number 97. Therefore, we expect the magnetic fields generated in the helical runs to be purely due to the action of a large-scale dynamo mechanism. The critical Reynolds number for the onset of the large-scale dynamo was observed to roughly double between the thermally stable versus unstable runs, the conclusion being that the thermal instability makes large-scale dynamo action more difficult. Whereas density and magnetic fields were observed to be almost completely uncorrelated in the thermally stable cases investigated, the action of thermal instability was observed to produce a positive correlation of the form B ∝ ρ0.2. This correlation is rather weak, and in addition it was observed to break down at the limit of highest densities.
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