Slow magnetosonic wave absorption by pressure induced ionization–recombination dissipation

T. Mishonov, A. Varonov
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引用次数: 1

Abstract

A new mechanisms for damping of slow magnetosonic waves (SMW) by pressure induced oscillations of the ionization degree is proposed. An explicit formula for the damping rate is quantitatively derived. Physical conditions where the new mechanism will dominate are briefly discussed. The ionization-recombination damping is frequency independent and has no hydrodynamic interpretation. Roughly speaking large area of partially ionized plasma are damper for basses of SMW while usual MHD mechanisms operate as a low pass filter. The derived damping rate is proportional to the square of the sine between the constant magnetic field and the wave-vector. Angular distribution of the spectral density of SMW and Alfven waves (AW) created by turbulent regions and passing through large regions of partially ionized plasma is qualitatively considered. The calculated damping rate is expressed by the electron impact cross section of the hydrogen atom and in short all details of the proposed damping mechanisms are well studied.
压力诱导电离复合耗散的慢磁声波吸收
提出了一种利用压力诱导的电离度振荡来衰减慢磁声波的新机制。定量地导出了阻尼率的显式公式。简要讨论了新机制将占主导地位的物理条件。电离复合阻尼与频率无关,没有水动力解释。粗略地说,大面积的部分电离等离子体是SMW基底的阻尼器,而通常的MHD机制作为低通滤波器。导出的阻尼率与恒定磁场和波矢量之间的正弦的平方成正比。定性地考虑了湍流区产生的SMW和Alfven波(AW)的谱密度角分布,并通过大面积的部分电离等离子体。计算出的阻尼率由氢原子的电子冲击截面表示,简而言之,所提出的阻尼机制的所有细节都得到了很好的研究。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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