Burgers方程的激波解与激波位置(英文)

讨论了Burgers方程激波解和位置的转移 .认为 :对该类方程 ,当边值发生微小变化时 ,不仅激波解发生变化 ,而且激波位置将发生较大的变化 ,甚至从内层移到边界 .其激波解也会发生相应的变化 .     

RLW-Burgers方程的一类解析解

本文给出了 RLW-Burgers方程及 Kd V-Burgers方程的一类解析解 ,且可得到 RLW-Burgers方程的振荡激波解 .这些解可以表示为 Burgers方程和 Kd V方程解的线性组合 ,文末还对文 [8]作了讨论 .     

一类非线性Burgers方程组的基于Hopf-Cole变换的直接间断Galerkin有限元方法

<正>1引言Burgers方程可以作为描述许多物理现象的数学模型,如交通流、激波、扰流问题和连续的随机过程.它还可以用于检验数值方法的效率.由于其具有较广的实用范围,一些学者对其近似解进行了较多的研究.如Adomian分解方法、混合有限差分和边界元方法、样条有限元方法、精确显式有限差分方法、Douglas有限差分格式,直接变分方法和变分迭代方法被用于Burgers方程近似解的研究~([1-13]).Hopf-Cole变换~([14,15])是研究Burgers方程较好的分析工具,利用它可以获得Burgers方程一些精确解.近年来,人们意识到该变换也是一个很好的数值工具并利用其得到了一     

指数同伦法对Cauchy条件下变系数Burgers方程的解析与数值分析

使用近似解析法来研究在给定初始条件和边界条件下变系数Burgers方程,引入一种新式同伦来解决微分方程中由变系数带来的问题,这种新同伦比传统方法计算更高效,并能给出时域上的一致解析表达式.分别计算了有限空间域上变系数Burgers方程的解析解,讨论了在有限空间区域上激波的形成,并对所得解析解进行了范数意义下收敛性研究的探索.基于Lie(李)变换群理论,研究了该方程的对称性质,给出了其无穷小生成子,守恒律和群不变解.文中给出的解是从非线性偏微分方程中直接得到的,未经过行波变换.通过"h-curve"准则探讨了近似解的收敛性.通过有限差分法进行直接数值模拟,已验证该方法的准确性和有效性.     

一类非线性边值问题解的激波性态

利用激波理论和匹配原理, 在适当的条件下讨论了一类非线性方程的激波问题, 得出了其激波解及其激波位置的表示式.将其结果用于一类可压缩流体流动模型, 较简捷地得到了该模型解的激波性态.     

一类拟线性边值问题的激波解

本文研究了一类拟线性边值问题的激波解，在适当的条件下，利用微分不等式理论，讨论了原边值问题激波解的存在性和渐近性态。     

变耗散系数的柱Burgers方程和球Burgers方程的精确解

根据简化齐次平衡原则,导出一个由线性方程的解到一个具变耗散系数的柱Burgers方程解的非线性变换.该线性方程容许有指数函数形式的解,因而借助所导出的非线性变换,获得一个具变耗散系数的柱Burgers方程的精确解.完全类似地,也获得一个具变耗散系数的球Burgers方程的精确解.     

非线性奇摄动两点边值问题的激波性态

在适当的条件下，利用奇摄动理论和匹配原理，讨论了一类非线性奇摄动两点边值问题的激波性态，构造了原问题的内部和外部解，较简捷地得到了与边界条件相对应的具有激波性态的解的表达式以及位于区间内部的激波位置。     

同伦分析法求解Burgers方程的初边值问题

采用同伦分析法求解了Burgers方程的一初边值问题,得到了它的近似解析解.在不同粘性系数情形下,对近似解与精确解进行了比较,发现在粘性系数不是非常小的情况下,用此方法得到的解析解与精确解符合地很好.     

非线性退化波方程的Riemann问题

研究了弹性力学中一退化波方程的Riemann问题．其应力函数非凸非凹,从而使得激波条件退化．通过引入广义激波条件下的退化激波,构造性地得到了各种情形下Riemann问题的整体解．     

KdVB方程行波解的定量分析

本文利用数学分析的方法、研究了v2≥4μ时KdVB方程的行波解.证明KdVB方程行波解与相应的Burgers方程行波解在定量方面的类似性.证明一般渐近展开式的截断误差是小参数ε的高阶量.     

有限变形弹性杆中的几何非线性波

利用有限变形理论的Lagrange描述,借助非保守系统的Hamilton型变分原理,导出了描述弹性杆中几何非线性波的波动方程．为了使非线性波动方程有稳定的行波解,计及了粘性效应引入的耗散和横向惯性效应导致的几何弥散．运用多重尺度法将非线性波动方程简化为KdV-Bergers方程,这个方程在相平面上对应着异宿鞍-焦轨道,其解为振荡孤波解．如果略去粘性效应或横向惯性,方程将分别退化为KdV方程或Bergers方程,由此得到孤波解或冲击波解,它们在相平面上对应着同宿轨道或异宿轨道．     

The Singular Structure of Non-selfsimilar Global Solutions of n Dimensional Burgers Equation

We investigate the singular structure for n dimensional non-selfsimilar global solutions and interaction of non-selfsimilar elementary wave of n dimensional Burgers equation, where the initial discontinuity is a n dimensional smooth surface and initial data just contain two different constant states, global solutions and some new phenomena are discovered. An elegant technique is proposed to construct n dimensional shock wave without dimensional reduction or coordinate transformation.     

Travelling waves for a non-local Korteweg–de Vries–Burgers equation

We study travelling wave solutions of a Korteweg–de Vries–Burgers equation with a non-local diffusion term. This model equation arises in the analysis of a shallow water flow by performing formal asymptotic expansions associated to the triple-deck regularisation (which is an extension of classical boundary layer theory). The resulting non-local operator is a fractional derivative of order between 1 and 2. Travelling wave solutions are typically analysed in relation to shock formation in the full shallow water problem. We show rigorously the existence of these waves. In absence of the dispersive term, the existence of travelling waves and their monotonicity was established previously by two of the authors. In contrast, travelling waves of the non-local KdV–Burgers equation are not in general monotone, as is the case for the corresponding classical KdV–Burgers equation. This requires a more complicated existence proof compared to the previous work. Moreover, the travelling wave problem for the classical KdV–Burgers equation is usually analysed via a phase-plane analysis, which is not applicable here due to the presence of the non-local diffusion operator. Instead, we apply fractional calculus results available in the literature and a Lyapunov functional. In addition we discuss the monotonicity of the waves in terms of a control parameter and prove their dynamic stability in case they are monotone.     

Exact traveling wave solutions of the Boussinesq–Burgers equation

The extended homogeneous balance method is used to construct exact traveling wave solutions of the Boussinesq–Burgers equation, in which the homogeneous balance method is applied to solve the Riccati equation and the reduced nonlinear ordinary differential equation. Many exact traveling wave solutions of the Boussinesq–Burgers equation are successfully obtained.     

Approximate inertial manifolds of Burgers equation approached by nonlinear Galerkin’s procedure and its application

The approximate inertial manifolds (AIMs) of Burgers equation is approached by nonlinear Galerkin methods, and it can be used to capture and study the shock wave numerically in a reduced system with low dimension. Following inertial manifolds, the asymptotic behavior of Burgers equation, an infinite dimensional dissipative dynamic systems, will evolve to a compact set known as a global attractor, which is finite-dimensional, and the nonlinear phenomena are included and captured in such global attractor. In the application, nonlinear Galerkin methods is introduced to approach such inertial manifolds. By this method, the solution of the original system is projected onto the complete space spanned by the eigenfunctions or the modes of the linear operator of Burgers equation, and nonlinear Galerkin method splits the infinite-dimensional phase space into two complementary subspaces: a finite-dimensional one and its infinite-dimensional complement. Then, the post-processed Galerkin’s procedure is used to approximate the solution of the reduced system, with the introduction of the interaction between lower and higher modes. Additionally, some numerical examples are presented to make a comparison between the traditional Galerkin method and nonlinear Galerkin method, in particular, some sharp jumping phenomena, which are related to the shock wave, have been captured by the numerical method presented. As the conclusion, it can be drawn that it is possible to completely describe the dynamics on the attractor of a nonlinear partial differential equation (PDE) with a finite-dimensional dynamical system, and the study can provide a numerical method for the analysis of the nonlinear continuous dynamic systems and complicated nonlinear phenomena in finite-dimensional dynamic system, whose nonlinear dynamics has been developed completely compared with infinite-dimensional dynamic system.     

Interaction Between Kink Solitary Wave and Rogue Wave for (2+1)-Dimensional Burgers Equation

Based on a suitable ansätz approach and Hirota’s bilinear form, kink solitary wave, rogue wave and mixed exponential–algebraic solitary wave solutions of (2+1)-dimensional Burgers equation are derived. The completely non-elastic interaction between kink solitary wave and rogue wave for the (2+1)-dimensional Burgers equation are presented. These results enrich the variety of the dynamics of higher dimensional nonlinear wave field.     

一类Burgers方程的孤立波解

Burgers方程在工程上有着重要的应用,它可以用来描述湍流、车队的交通流、氏族的随机迁移、化学工程中的分离等现象,对Burgers方程求解方法的研究有着重要的现实意义.对Burgers方程求解主要是应用差分和微分两方面的方法来展开求解的,1/G展开法是近年来发展起来的求解非线性偏微分方程的一种较为有效的微分解法.采用微分方程方面的方法,利用1/G展开法对一类Burgers方程进行求解,得到了此方程的一类孤立波解和扭曲波解,同时描绘出解的图像并分析解的结构和变化趋势.     

A new derivation of Painlevé hierarchies

We give a new derivation of two Painlevé hierarchies. This is done by extending the accelerating-wave reductions of the Korteweg-de Vries and dispersive water wave equations to their respective hierarchies. We also consider the extension of this reduction of Burgers equation to the Burgers hierarchy.     

Bildung schwacher stationärer Stosswellen in relaxierenden Gasgemischen

Summary The formation of a fully dispersed shock wave in a binary mixture of relaxing gases is investigated. It is assumed that the gas is bounded by a piston at the left, and at timet=0 is in static thermodynamic equilibrium. The piston velocity changes from zero att=0 to a constant non-zero value att>0. A uniformly valid approximation for the resulting wave motion is found by the method of matched asymptotic expansions. It turns out that the formation of a steady shock wave depends on the temperature dependence of the vibrational specific heats. If the coefficient of the non-linear term in Burgers equation is greater than zero, a steady shock wave is formed. However, for 0 this is not the case. One finds that the cases 0 are not realized in nature. Numerical results for the shock formation in relaxing air indicate, how the accuracy of acoustic theory decreases due to non-linear effects as time proceeds.