超越拟线性近似的电子尾碰撞不稳定性中的弛豫机制

D. W. Crews, U. Shumlak
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引用次数: 0

摘要

利用拟线性理论和直接Vlasov-Poisson模拟的高阶不连续伽辽金方法,对电子尾碰撞不稳定性进行了数值研究,这是理解无碰撞松弛过程和异常电阻率的经典模型问题。拟线性扩散最初与直接模拟很好地吻合,但后来低估了湍流动量通量。当最大振幅波包中的相空间涡流周转时间与共振相流体的波包传递时间相当时,磁通增强。在这种状态下,涡流在波包传输过程中有效地翻转,使得相流体主要通过涡流相混合而不是随机相波来分散。结果是比拟线性预测的弛豫率提高了。这些发现提供了一种方法来理解准线性扩散理论和观察到的空间和实验室等离子体波动的比较背后的物理。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Mechanism Of Relaxation In The Electron Bump-On-Tail Instability Beyond The Quasilinear Approximation
The electron bump-on-tail instability, a classic model problem to understand collisionless relaxation processes and anomalous resistivity, is studied numerically using high-order discontinuous Galerkin methods applied to both quasilinear theory and direct Vlasov-Poisson simulation. Quasilinear diffusion is initially in good agreement with a direct simulation but later underestimates turbulent momentum flux. Enhanced flux occurs as the phase space eddy turnover time in the largest amplitude wavepackets becomes comparable to the wavepacket transit time of resonant phase fluid. In this regime eddies effectively turn over during wavepacket transit so that phase fluid predominately disperses by eddy phase mixing rather than by randomly phased waves. The result is an enhanced rate of relaxation above quasilinear predictions. These findings provide a means to understand the physics behind comparisons of quasilinear diffusion theories and observed fluctuations in space and laboratory plasmas.
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