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Resonant surface waves and instabilities in finite beta plasmas

机译:有限β等离子体中的共振表面波和不稳定性

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Magnetohydrodynamic surface waves are studied at an interface of finite thickness separating two homogeneous arbitrary finite beta plasmas which are in parallel motion with respect to each other and are permeated by parallel magnetic fields. It is assumed that the density decreases and the magnetic field strength increases across the interface. The model is representative of the mantle-like boundary layer separating the fast flowing magnetosheath from the tail region of the magnetosphere. All existing wave modes are classified, their main properties are investigated, and analytical expressions for critical velocities are obtained. The resonant flow instability (RFI) and Kelvin-Helmholtz instability are studied when the finite thickness of the inhomogeneous boundary layer is taken into account. The theory of negative energy waves is applied to predict the behavior and interactions of the surface modes in such plasmas. Growth rates of RFIs are examined under various conditions. The dependence of critical velocities on the density ratio is studied under the assumption of a nonuniform magnetic field resulting in different plasma 8 on both sides of the inhomogeneous layer. Possible observational signatures of the RFI are also discussed. (C) 2003 American Institute of Physics. [References: 31]
机译:磁流体动力学表面波是在有限厚度的界面处研究的,该界面将两个相互平行运动且被平行磁场渗透的均质任意有限β等离子体隔开。假设在界面上密度降低而磁场强度增加。该模型代表了地幔状边界层,该边界层将快速流动的磁荒与磁层的尾部区域分开。对所有现有的波模进行分类,研究其主要性质,并获得临界速度的解析表达式。当考虑非均匀边界层的有限厚度时,研究了共振流动不稳定性(RFI)和开尔文-亥姆霍兹不稳定性。负能波理论被用于预测这种等离子体中表面模式的行为和相互作用。在各种条件下检查RFI的增长率。在不均匀磁场的假设下研究临界速度对密度比的依赖性,该磁场导致在不均匀层的两侧上存在不同的等离子体8。还讨论了RFI的可能的观测特征。 (C)2003美国物理研究所。 [参考:31]

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