Klein–Gordon equation and reflection of Alfvén waves in nonuniform media

Z. Musielak, J. Fontenla, R. Moore
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引用次数: 39

Abstract

A new analytical approach is presented for assessing the reflection of linear Alfven waves in smoothly nonuniform media. The general one‐dimensional case in Cartesian coordinates is treated. It is shown that the wave equations, upon transformation into the form of the Klein–Gordon equation, display a local critical frequency (Ωc) for reflection: At any location in the medium, reflection becomes strong as the wave frequency descends past this characteristic frequency set by the local nonuniformity of the medium. This critical frequency is given by the transformation as an explicit function of the Alfven velocity (VA), and its first (V’A) and second (V■A) derivatives, and hence as an explicit spatial function. The transformation thus directly yields, without solution of the wave equations, the location in the medium at which an Alfven wave of any given frequency becomes strongly reflected and has its propagation practically cut off. The local critical frequency is the square root of the larger coefficient o...
Klein-Gordon方程与非均匀介质中alfvsamn波的反射
提出了一种新的计算线性阿尔芬波在光滑非均匀介质中的反射的解析方法。在笛卡尔坐标系中处理一般的一维情况。结果表明,波动方程在转换为Klein-Gordon方程后,显示出一个局部反射临界频率(Ωc):在介质中的任何位置,当波频率下降到超过由介质的局部非均匀性设定的特征频率时,反射变得强烈。这个临界频率由变换给出,作为阿尔芬速度(VA)及其一阶导数(V 'A)和二阶导数(V■A)的显式函数,因此作为显式空间函数。因此,这种变换直接产生了在介质中的某个位置,在这个位置上,任何给定频率的阿尔芬波都被强烈反射,其传播几乎被切断,而无需求解波动方程。局部临界频率是较大系数o的平方根…
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