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Contributions to the theory of magnetorotational instability and waves in a rotating plasma

机译:对磁旋转定律和旋转等离子体中的波理论的贡献

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The one-fluid magnetohydrodynamic (MHD) theory of magnetorotational instability (MRI) in an ideal plasma is presented. The theory predicts the possibility of MRI for arbitrary 0, where 0 is the ratio of the plasma pressure to the magnetic field pressure. The kinetic theory of MRI in a collisionless plasma is developed. It is demonstrated that as in the ideal MHD, MRI can occur in such a plasma for arbitrary P. The mechanism of MRI is discussed; it is shown that the instability appears because of a perturbed parallel electric field. The electrodynamic description of MRI is formulated under the assumption that the dispersion relation is expressed in terms of the permittivity tensor; general properties of this tensor are analyzed. It is shown to be separated into the nonrotational and rotational parts. With this in mind, the first step for incorporation of MRI into the general theory of plasma instabilities is taken. The rotation effects on Alfven waves are considered.
机译:提出了理想等离子体中的磁旋转不稳定性(MRI)的单流体磁流体动力学(MHD)理论。该理论预测MRI取任意0的可能性,其中0是等离子压力与磁场压力之比。建立了无碰撞等离子体中MRI的动力学理论。已证明,与理想的MHD一样,对于任意P,血浆中均可发生MRI。结果表明,不稳定性是由于扰动的平行电场而出现的。 MRI的电动力学描述是在假设色散关系用介电常数张量表示的前提下制定的。分析了该张量的一般性质。它显示为分为非旋转部分和旋转部分。考虑到这一点,迈出了将MRI纳入血浆不稳定性一般理论的第一步。考虑了对Alfven波的旋转效应。

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