Two-stream instability

北尾 一夫
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引用次数: 1

Abstract

For an introduction to the instability, see Chapter 6.6 of the plasma physics textbook by Chen. We imagine a plasma with cold electrons moving relative to cold ions. The dispersion relation is 1 F k ω  ()  0  where F k ω  () ω pe 2 ω k v   () 2 ω pi 2 ω 2   The little black boxes indicate that evaluation has been disabled. Let's give the variables some values: ω pe 10  ω pi 10  k 1  v 20  F k ω  () ω pe 2 ω k v   () 2 ω pi 2 ω 2   Now we plot this function using  values that miss the singularities. We make two plots, one with k = 1 and one with k = 2. Also we plot a line one unit above zero.
二束不稳定
关于不稳定性的介绍,请参见Chen编写的等离子体物理教科书第6.6章。我们想象一个等离子体,它的冷电子相对于冷离子运动。色散关系为1 F k ω ()其中F k ω ()ω pe 2 ω k v () 2 ω pi 2 ω 2小黑盒子表示已禁用评估。让我们给这些变量一些值:ω pe 10ω pi 10k 1v 20F k ω ()ω pe 2 ω k v () 2 ω pi 2 ω 2现在我们使用值来绘制这个函数,这些值忽略了奇点。我们画两个图,一个是k = 1,另一个是k = 2。我们还画了一条直线在零上方一个单位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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