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Anomalous temperature relaxation and particle transport in a strongly non-uniform, fully ionized plasma in a strong magnetic field

机译:在强磁场中强烈不均匀,完全电离的等离子体中的异常温度松弛和粒子传输

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摘要

In classical kinetic and transport theory for a fully ionized plasma in a magnetic field, collision integrals from a uniform theory without fields are uaed, When the magnetic field is so strong that electrons may gyrate during electron-electron and, electron-ion interactions, the form of the collision integrals will be modified, Another modification will stem from strong non-uniformities transverse to the magnetic field B. Using collision terms that explicitly incorporate these effects, we derive in particular the temperature relaxation between electrons and ions and the particle transport transverse to the magnetic field. In both cases collisions between gyrating electrons, which move along the magnetic field, and non-gyrating ions, .which move , in arbitrary directions at a distance transverse to B from the electrons larger than the electron, Larmor radius but smaller than the Debye l0ngth? give rise to enhancement factors in the corresponding classical expressions of order In (M_(ion)/M_(el)).
机译:在磁场中完全电离的等离子体的经典动力学和输运理论中,使用了没有场的均匀理论的碰撞积分。当磁场如此强,以至于电子在电子与电子相互作用期间可能发生旋转时,碰撞积分的形式将被修改,另一种修改将来自于垂直于磁场B的强不均匀性。使用明确包含这些效应的碰撞项,我们尤其得出了电子和离子之间的温度弛豫以及粒子传输的横向磁场。在这两种情况下,沿磁场运动的旋转电子与非旋转离子之间的碰撞在沿大于B的电子的任意方向上以任意方向移动,该距离大于电子,拉莫尔半径但小于Debye 10ngth ?在(M_(ion)/ M_(el))阶的相应经典表达式中产生增强因子。

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