首页> 外文期刊>Journal of Geophysical Research. Biogeosciences >Stabilization of lower-hybrid drift instability in the magnetotail by finite north-south magnetic field component and destabilization by sheared cross-field flow
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Stabilization of lower-hybrid drift instability in the magnetotail by finite north-south magnetic field component and destabilization by sheared cross-field flow

机译:有限的南北磁场分量稳定磁尾中的下混合漂移不稳定性,并通过剪切交叉场流使失稳失稳

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The problem of nonlocal lower-hybrid drift instability in the magnetotail-like geometry characterized by a finite north-south;(normal) magnetic field component at the center of the neutral sheet is revisited. In a preliminary paper [Lui et al., 1995] it was shown that the one-dimensional neutral sheet of the Harris type with constant cross-held flow speed profile, v = v(0) = const, is stable with respect to perturbations in the lower-hybrid frequency range, if the normal field component is finite, B-n > 0. They then discussed a sheared flow speed profile, v(z) = v(0)/[1+(z/Delta)(2)], which represents a much thinner current sheet configuration, and recovered the unstable mode. In this paper, the previous work is extended in two aspects. The effects of the variation of the normal field strength, B-n, on the transition from instability to stability in the absence of the shear (Delta = infinity) is examined systematically. In addition, the eigenmodes with odd symmetry, phi(-z) = -phi (z), are included. These two extensions Show that indeed, the normal field component B-n has a strong stabilizing influence on the mode. As the shear parameter Delta is reduced, the threshold value of B-n for stabilization increases in proportion to the value of Delta (-1), which leads to the conclusion that the shear in the cross-field drift speed has a destabilizing influence on the mode. Comparison of the two symmetry modes shows that the odd symmetry eigenmodes generally possess higher growth rates than the even symmetry ones. [References: 50]
机译:再次探讨了以中性薄板中心为特征的南北(法向)磁场分量为特征的磁尾状几何形状中的非局部下混合漂移不稳定性问题。在一份初步论文中[Lui et al。,1995],表明具有恒定交叉保持流速分布的哈里斯型一维中性片相对于扰动是稳定的,v = v(0)= const。在低混合频率范围内,如果法向场分量是有限的,则Bn>0。然后他们讨论了剪切流速分布,v(z)= v(0)/ [1+(z / Delta)(2)表示较薄的当前工作表配置,并恢复了不稳定模式。在本文中,先前的工作在两个方面进行了扩展。系统地研究了法向场强B-n的变化对在不存在剪切力的情况下从不稳定性过渡到稳定性的影响(Δ=无穷大)。此外,还包括具有奇对称性的本征模phi(-z)= -phi(z)。这两个扩展表明,确实,法向场分量B-n对模式具有很强的稳定影响。随着剪切参数Delta的减小,用于稳定的Bn阈值与Delta(-1)的值成比例地增加,从而得出结论,即跨场漂移速度中的剪切力对振型有不稳定的影响。 。两种对称模式的比较表明,奇数对称本征模式通常具有比偶数对称本征模式更高的增长率。 [参考:50]

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