论通过较简单线性或非线性微分方程的解来获取非线性微分方程的解

Nikolay K. Vitanov
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引用次数: 0

摘要

在本文中,我们遵循一种与霍普夫和科尔相反的思想:我们利用变换来将较简单的线性或非线性微分方程(已知解)变换为较复杂的非线性微分方程。通过这种方法,我们可以得到许多非线性微分方程的精确解。我们将这一方法应用于经典抛物微分方程(波方程)、经典双曲微分方程(热方程)和经典椭圆微分方程(拉普拉斯方程)。此外,我们还通过线性微分方程的解以及伯努利和里卡提非线性微分方程的解,利用这些方法获得非线性常微分方程的精确解。最后,我们展示了该方法在其他非线性偏微分方程已知解的基础上得出非线性偏微分方程精确解的能力。本文特别关注非线性微分方程的行波解。我们证明了所得到的一些解所描述的以下现象的存在:(i) 解中出现孤波-孤反波,在初始时刻为零(类似于真空中出现的粒子和反粒子);(ii) 非线性孤波分裂为两个孤波(类似于一个粒子分裂为两个粒子);(iii) 部分所得波的孤子行为;(iv) 尽管孤子的形状和振幅不同,但存在以相同速度运动的孤子。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the Obtaining Solutions of Nonlinear Differential Equations by Means of the Solutions of Simpler Linear or Nonlinear Differential Equations
In this article, we follow an idea that is opposite to the idea of Hopf and Cole: we use transformations in order to transform simpler linear or nonlinear differential equations (with known solutions) to more complicated nonlinear differential equations. In such a way, we can obtain numerous exact solutions of nonlinear differential equations. We apply this methodology to the classical parabolic differential equation (the wave equation), to the classical hyperbolic differential equation (the heat equation), and to the classical elliptic differential equation (Laplace equation). In addition, we use the methodology to obtain exact solutions of nonlinear ordinary differential equations by means of the solutions of linear differential equations and by means of the solutions of the nonlinear differential equations of Bernoulli and Riccati. Finally, we demonstrate the capacity of the methodology to lead to exact solutions of nonlinear partial differential equations on the basis of known solutions of other nonlinear partial differential equations. As an example of this, we use the Korteweg--de Vries equation and its solutions. Traveling wave solutions of nonlinear differential equations are of special interest in this article. We demonstrate the existence of the following phenomena described by some of the obtained solutions: (i) occurrence of the solitary wave--solitary antiwave from the solution, which is zero at the initial moment (analogy of an occurrence of particle and antiparticle from the vacuum); (ii) splitting of a nonlinear solitary wave into two solitary waves (analogy of splitting of a particle into two particles); (iii) soliton behavior of some of the obtained waves; (iv) existence of solitons which move with the same velocity despite the different shape and amplitude of the solitons.
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