Burgers方程的数值解(Ⅰ)

引言 近年来,越来越多的工作从事于非线性格式的计算稳定性(见[1]—[6]).作者提出了非线性格式广义稳定性的概念并提供了估计非线性格式误差的一系列技巧(见[7]—[9]).这些方法已广泛应用到许多问题.例如,涡度方程(见[10]—[12]),Navier-Stokes方程(见[13]—[16]),可压缩流体(见[17]),大气环流方程(见[18]—[20]),K.D.V方程(见[21]—[23])和非线性波动方程(见[24]—[25]).本文以下列Burgers方程为例来介绍这一方法:     

高阶中立型方程渐近稳定性的代数判定

微分差分方程渐近稳定性的代数判据在应用时比较方便。最近,文[1]给出了滞后型方程渐近稳定的代数判据,文[2]给出了一阶中立型方程渐近稳定的代数判据。本文旨在推广文[2]的结果,给出高阶中立型方程渐近稳定的代数判据。 考虑中立型微分差分方程     

用Fourier方法解半线性抛物型方程双移动边界问题

文[1]就金属板烧蚀中提出的问题,给出了热导方程单个移动边界问题的Fourier型级数求解法。文[2]研究了热导方程双移动边界问题。还有些人研究了抛物型方程移动边界问题情况。但是迄今这一类问题的研究工作集中于线性的情况,对非线性的情况讨论甚少,其它移动边界问题也是如此(参见[3]、[4])。本文是在[1]、[2]的基础上,讨论如下的一类半线性抛物型方程双移动边界的定解问题:     

无限相似单元法的收敛性

[1]与[2、3]相互独立地提出了无限相似单元法。[2、3]讨论了拉普拉斯方程在有角点区域上的奇性解。[1]讨论了平面弹性力学方程组的奇性解及其对应的应力强度因子,但[1]中的方法对于包括拉普拉斯方程在内的一类椭圆型方程都是适用的。这一方法还可以推广到无界区域上去,这部分内容将在另文中讨论。     

离散椭圆型方程的矩阵方程表示及其直接解法

在[1]中讨论了解离散椭圆型方程的直接法,[2]、[3]中在椭圆型方程的类型和区域上得到了进一步的推广.它们的优点是计算起来快速且仅需要极小的存贮量.本文把求解的线性方程组写成矩阵方程形式,进一步发展矩阵分解法.首先,为了简单,如[1]那样考虑方程组     

二维非线性对流-扩散方程的特征-差分解法

1.引言 近年来,求解对流-扩散方程的修正特征线法日渐被人们重视,已有不少人讨论了这一方法,如[1]-[5]。其中[1]和[2]是该领域的奠基性工作。[6]讨论了对流-扩散方程的特征-差分方法,改善并推广了[1]中某些重要结果。本文将讨论二维非线性对流-扩     

二阶拟线性椭圆型方程一般边值问题解的存在性

在文章[1]与[2]中,曾用了不同的方法证明一个空间变量的拟线性抛物型方程一般边值问题解的存在定理.本文利用与[1]相类似的方法考虑多个自变量椭圆型方程一般边值问题     

确定抛物线位置的简捷方法

所见书刊都是先用坐标变换等理论,将一般二次曲线方程化简为标准方程,从而确定曲线形状和位置的,如文[1]是用“基本不变量”化简方程确定曲线的位置;而文[2]是用二次曲线的直径方程研     

关于“几类具5次强非线性项的发展方程的显式精确孤波解”的注记

关于非线性发展方程的孤波解问题一直是人们感兴趣的一个研究课题 .本文指出文 [2 ]中关于Kundu方程和导数 Schr dinga方程的结论事实上是可以用积分法得到 ,而且文 [1 ,2 ]中涉及到的其它非线性发展方程的相应结论 ,用积分法也能得到     

在分子晶体激子中的一类非线性Schrdinger方程组的初值和周期初值问题

最近发表了一系列文章,其中指明在类Schrdinger方程基础上可以处理在固体中的各种激发,特别提到了在一维晶体中[2,3,4]和α—螺旋生物分子中[5]产生的激子(exciton).在[4,6]中指出这类方程的经典形式为     

推广的KdV方程特征问题解的存在唯一性

推广的KdV方程u_t+αuu_x+μu_x3+εu_x5=0[1]是典型的可积方程.它先后在研究冷等离子体中磁声波的传播[2],传输线中孤立波[3]和分层流体中界面孤立波[4]时导出.本文对推广的KdV方程的特征问题,在Riemann函数的基础上,设计一恰当结构,并由此化待征问题为一与之等价的积分微分方程.而该积分微分方程对应的映射E是列自身的映射[5],依不动点原理,积分微分方程有唯一的正则解,即推广的KdV方程的特征问题有唯一解,且由积分微分方程序列所得的迭代解于Ω上一致收敛.     

Nonfocusing Instabilities in Coupled, Integrable Nonlinear Schrödinger pdes

nonfocusing instabilities that exist independently of the well-known modulational instability of the focusing NLS equation. The focusing versus defocusing behavior of scalar NLS fields is a well-known model for the corresponding behavior of pulse transmission in optical fibers in the anomalous (focusing) versus normal (defocusing) dispersion regime [19], [20]. For fibers with birefringence (induced by an asymmetry in the cross section), the scalar NLS fields for two orthogonal polarization modes couple nonlinearly [26]. Experiments by Rothenberg [32], [33] have demonstrated a new type of modulational instability in a birefringent normal dispersion fiber, and he proposes this cross-phase coupling instability as a mechanism for the generation of ultrafast, terahertz optical oscillations. In this paper the nonfocusing plane wave instability in an integrable coupled nonlinear Schr?dinger (CNLS) partial differential equation system is contrasted with the focusing instability from two perspectives: traditional linearized stability analysis and integrable methods based on periodic inverse spectral theory. The latter approach is a crucial first step toward a nonlinear , nonlocal understanding of this new optical instability analogous to that developed for the focusing modulational instability of the sine-Gordon equations by Ercolani, Forest, and McLaughlin [13], [14], [15], [17] and the scalar NLS equation by Tracy, Chen, and Lee [36], [37], Forest and Lee [18], and McLaughlin, Li, and Overman [23], [24]. Received February 9, 1999; accepted June 28, 1999     

Algebraic travelling waves for the generalized Burgers-Fisher equation

Abstract

Using the definition of algebraic travelling wave solution for general 2-th order differential equations given in [9], we provide the only possible algebraic travelling wave solutions for the celebrated generalized Burgers-Fisher equation.     

Weighted Strichartz estimates for the wave equation in even space dimensions

We prove the weighted Strichartz estimates for the wave equation in even space dimensions with radial symmetry in space. Although the odd space dimensional cases have been treated in our previous paper [5], the lack of the Huygens principle prevents us from a similar treatment in even space dimensions. The proof is based on the two explicit representations of solutions due to Rammaha [11] and Takamura [14] and to Kubo-Kubota [6]. As in the odd space dimensional cases [5], we are also able to construct self-similar solutions to semilinear wave equations on the basis of the weighted Strichartz estimates.Mathematics Subject Classification (2000): 35L05, 35B45, 35L70COE fellowDedicated to Professor Mitsuru Ikawa on the occasion of his sixtieth birthday     

Solitary wave solutions for high dispersive cubic-quintic nonlinear Schrödinger equation

We consider the higher-order dispersive nonlinear Schrödinger equation including fourth-order dispersion effects and a quintic nonlinearity. This equation describes the propagation of femtosecond light pulses in a medium that exhibits a parabolic nonlinearity law. By adopting the ansatz solution of Li et al. [Zhonghao Li, Lu Li, Huiping Tian, Guosheng Zhou. New types of solitary wave solutions for the higher-order nonlinear Schrödinger equation. Phys Rev Lett 2000;84:4096], we find two different solitary wave solutions under certain parametric conditions. These solutions are in the form of bright and dark soliton solutions.     

A FLUID-PARTICLE MODEL WITH ELECTRIC FIELDS NEAR A LOCAL MAXWELLIAN WITH RAREFACTION WAVE

The paper is concerned with time-asymptotic behavior of solution near a local Maxwellian with rarefaction wave to a fluid-particle model described by the Vlasov-Fokker-Planck equation coupled with the compressible and inviscid fluid by Euler-Poisson equations through the relaxation drag frictions, Vlasov forces between the macroscopic and microscopic momentums and the electrostatic potential forces. Precisely, based on a new micro-macro decomposition around the local Maxwellian to the kinetic part of the fluid-particle coupled system, which was first developed in [16], we show the time-asymptotically nonlinear stability of rarefaction wave to the one-dimensional compressible inviscid Euler equations coupled with both the Vlasov-Fokker-Planck equation and Poisson equation.     

Nonlinear waves in friedman-robertson-walker space-times

In this paper we consider the initial value problem for the nonlinear wave equation □u = F(u, u′) in Friedman-Robertson-Walker space-time, □ being the D'Alambertian in local coordinates of space-time. We obtain decay estimates and show that the equation has global solutions for small initial data. We do it by reducing the problem to an initial value problem for the wave equation over hyperbolic space. As byproduct we derive decay and global existence for solutions of the wave equation over the hyperbolic space with small initial data. The same technique with some auxiliary lemmas similar to the ones proved in [6], [7] can be used to generalize the result to the case when F depends also on second derivatives of u in a certain way.     

A note on “New travelling wave solutions to the Ostrovsky equation”

In a recent paper by Ya?ar [E. Ya?ar, New travelling wave solutions to the Ostrovsky equation, Appl. Math. Comput. 216 (2010), 3191-3194], ‘new’ travelling-wave solutions to the transformed reduced Ostrovsky equation are presented. In this note it is shown that some of these solutions are disguised versions of known solutions.     

Global conservative solutions for a model equation for shallow water waves of moderate amplitude

In this paper, we study the continuation of solutions to an equation for surface water waves of moderate amplitude in the shallow water regime beyond wave breaking (in [11], Constantin and Lannes proved that this equation accommodates wave breaking phenomena). Our approach is based on a method proposed by Bressan and Constantin [2]. By introducing a new set of independent and dependent variables, which resolve all singularities due to possible wave breaking, the evolution problem is rewritten as a semilinear system. Local existence of the semilinear system is obtained as fixed points of a contractive transformation. Moreover, this formulation allows one to continue the solution after collision time, giving a global conservative solution where the energy is conserved for almost all times. Finally, returning to the original variables, we obtain a semigroup of global conservative solutions, which depend continuously on the initial data.     

A Method for Solving Exact Solution to Two－dimensional Korteweg－de Vires－Burgers Equation

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