带有非麦克斯韦电子和正电子的电子-正电子-离子等离子体中的球形和圆柱形离子声孤波

Sukhjeet Kaur
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引用次数: 2

摘要

研究了圆柱形和球形离子声孤波在由离子、电子和正电子组成的等离子体系统中的传播。假设电子和正电子遵循一般称为Tsallis分布的非广泛分布。采用适当的数学变换,对标准非线性方程即KdV方程进行了数值求解。本文用数值方法研究了非广泛性(q)和非平面几何对离子声势结构振幅和宽度的影响。在−1 < q < 0范围内较低的q值下,平面和非平面几何结构都观察到从负电位结构到正电位结构的转变。对于球形波,孤子振幅最大;对于平面波,孤子振幅最小;对于圆柱形波,孤子振幅介于两者之间。本研究有助于我们理解天体物理等离子体中柱面和球面孤立波的研究。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spherical and Cylindrical Ion Acoustic Solitary Waves in Electron-Positron-Ion Plasmas with Non-Maxwellian Electrons and Positrons
The propagation of cylindrical and spherical ion acoustic solitary waves in a plasma system consisting of ions, electrons and positrons are investigated. The electrons and positrons are assumed to be following the nonextensive distribution popularly known as Tsallis distribution. The standard nonlinear equation i.e. Korteweg de-Vries (KdV) equation has been solved numerically using suitable mathematical transformations. The effect of nonextensivity (q) and nonplanar geometry on the amplitudes and width of ion acoustic potential structures have been studied numerically. A transition from negative to positive potential structures have been observed for the planar as well as nonplanar geometries for lower values of q in the range −1 < q < 0. Soliton amplitude is maximum for spherical waves and is minimum and for planar waves while it lies in between the two for cylindrical waves. The present investigation may help us in understanding the study of cylindrical and spherical solitary waves in astrophysical plasmas.
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