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Two-component description of dynamical systems that can be approximated by solitons: The case of the ion acoustic wave equations of plasma physics

机译:可以用孤子近似的动力学系统的两部分描述:等离子物理的离子声波方程式的情况

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摘要

A new approach to the perturbative analysis of dynamical systems, which can be described approximately by soliton solutions of integrable non-linear wave equations, is employed in the case of small-amplitude solutions of the ion acoustic wave equations of plasma physics. Instead of pursuing the traditional derivation of a perturbed KdV equation, the ion velocity is written as a sum of two components: elastic and inelastic. In the single-soliton case, the elastic component is the full solution. In the multiple-soliton case, it is complemented by the inelastic component. The original system is transformed into two evolution equations: An asymptotically integrable Normal Form for ordinary KdV solitons, and an equation for the inelastic component. The zero-order term of the elastic component is a single-soliton or multiple-soliton solution of the Normal Form. The inelastic component asymptotes into a linear combination of single-soliton solutions of the Normal Form, with amplitudes determined by soliton interactions, plus a second-order decaying dispersive wave. Satisfaction of a conservation law by the inelastic component and of mass conservation by the disturbance to the ion density is determined solely by the initial data and/or boundary conditions imposed on the inelastic component. The electrostatic potential is a first-order quantity. It is affected by the inelastic component only in second order. The charge density displays a triple-layer structure. The analysis is carried out through the third order.
机译:在等离子体物理的离子声波方程的小振幅解的情况下,采用了一种新的动力学系统微扰分析方法,该方法可以用可积分非线性波动方程的孤子解近似描述。代替追求扰动KdV方程的传统推导,将离子速度写为两个分量之和:弹性和非弹性。在单孤子情况下,弹性分量是完整的解。在多孤子情况下,它由非弹性成分补充。原始系统被转换为两个演化方程:一个用于普通KdV孤子的渐近可积正态形式,一个用于非弹性分量的方程。弹性分量的零阶项是标准形式的单孤子或多孤子解决方案。非弹性分量渐近成为标准形式的单孤子解的线性组合,其振幅由孤子相互作用确定,外加二阶衰减色散波。非弹性组分对守恒定律的满意程度和离子密度的扰动对质量守恒的满意程度仅由施加在非弹性组分上的初始数据和/或边界条件确定。静电势是一阶量。它仅受二阶非弹性分量的影响。电荷密度显示三层结构。分析是通过三阶进行的。

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