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A possible excitation mechanism for a longitudinal wave iiiistaility in a plasma by a quasi-static electric field

机译:准静态电场在等离子体中产生纵波失稳的可能激发机制

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摘要

A specific type, of longitudinal wave instability in a plasma due entirely to an external quasi-static electric field Eo is considered for the oases of ion-acoustic and Langmuir waves. The quasi-static time variation of the field leads to a relal ively simple mechanism for the development, of instability. For frequency ranges typical.of ion-acoustic, and Langrauirwaves dispersion relations are obtained, with Landau damping and pair Coulomb collisions taken into account in addition to E(). The model integral of Bhatnagar, Gross & Krook is used to describe collisions. Two methods for taking account of the influence of the electric field on development of the instability are compared: that of Pines & Hchrieffer and that of Brinca and Dysthe. Expressions are obtained for the growth rates in the framework of linear theory. Numerical .simulations of both types of instabilities.are peiforined for specific values of the phisma parameters.
机译:对于离子声波和朗缪尔波的绿洲,可以考虑一种特定类型的,完全由外部准静态电场Eo引起的等离子体中的纵向波不稳定性。磁场的准静态时间变化会导致相对不稳定的发展机制。对于典型的频率范围,获得了离子声和朗格劳尔波的色散关系,除了E()外还考虑了兰道阻尼和成对库仑碰撞。 Bhatnagar,Gross&Krook的模型积分用于描述碰撞。比较了两种考虑电场对不稳定性影响的方法:Pines&Hchrieffer以及Brinca和Dysthe。在线性理论的框架内获得增长率的表达式。对于等离子参数的特定值,对两种类型的不稳定性进行了数值模拟。

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