具有平方、立方非线性项的耦合动力学系统1∶2内共振分岔

对一类具有平方、立方非线性项的耦合动力学系统1∶2内共振情形进行了研究A *D2首先,用直接方法求出该系统1∶2内共振时的Normal Form,该系统的Normal Form中,不仅含有平方非线性项,同时还含有立方非线性项A *D2通过采用适当的变量变换,将4维分岔方程约化成3维,进而得到单变量4次分岔方程A *D2最后用奇异性理论,研究了一类普适开折的分岔特性A *D2该方法可用于4维中心流形上流的强内共振时的分岔行为分析A *D2     

参数展开摄动法

本文提出一个参数展开摄动法,作为一个应用,讨论了非线性项上带有的参数不是很小时的一般Duffing方程的解。求得了解的渐近展开式。 本文还讨论了广义Duffing方程λ~2x+ex~3=O,这个方程不宜用寻常的摄动法求其渐近解,但用参数展开摄动法可以求其渐近解,文中构造了解的渐近形式,提出了二次近似与一次近似渐近解的稳定判据。     

一类变系数非线性奇摄动方程的变形坐标法

利用变形坐标法,讨论了一类变系数的非线性奇摄动问题:(xn+εym)dy/dx+nxn-1y=1,y(1)=a>1,x∈[0,1],0<ε<<1,m,n为自然数,a为常数.通过与L-P方法的对比和对参数几种不同取值的分类探讨,得到了该变系数非线性奇摄动方程的一致有效的渐近解.并且通过数值模拟,证实了方程的精确解和用变形坐标法得到的渐近解的一致性,从而说明用变形坐标法解此类奇摄动方程的渐近解的有效性.     

具有平方、立方非线性项的耦合动力学系统1：2内共振分贫

对一类具有平方,立方非线性项的耦合动力学系统1：2内共振情形进行了研究,首先,用直接方法求出该系统1：2内共振时的Normal Form,该系统的Normal Form中,不仅含有平方非线性项,同时还含有立方非线性项,通过采用适当的变量变换,将4维分贫方程约化成3维,进而得到单变量4次分岔方程,最后用奇异性理论,研究了一类普适开折的分岔特性,该方法可用于4维中心流形上流的强内共振时的分岔行为分析。     

多自由度非线性振动系统的多频分叉

本文研究自治和非自治多目由度非线性振动系统当其线化系统有多个特征值同时经过虚轴时产生的多频分叉问题,提出了用于分析多频分叉问题的平均摄动解法,得到了在共振和非共振情形的多频分叉渐近摄动解和稳定性判据,我们还将本文方法用在分析机车轮对动力系统的Hopf分叉中和Van der PolDuffing耦合非线性振子的双频分叉中。     

一类单自由度非自治系统的非线性振动

本文用奇异摄动理论多尺度法的导数展开法[1],求解了在微粘性阻尼作用下,连结在一个非线性弹簧上的一个质点的受迫振动方程.研究的是四次非线性问题,讨论了四种情况:非共振的软激发;非共振的硬激发;共振的软激发;共振的硬激发.     

一类非线性奇摄动方程的匹配解法和解的精度估计

利用匹配渐近展开法,研究了一类非线性奇异摄动方程.在适当的条件下,得出了该类问题解的渐近展开式.并将结果应用于例子,对渐近解与精确解和用两变量方法求得的解进行比较,可知所得到的渐近解达到了较高精度.     

双参数非线性非局部奇摄动抛物型初始-边值问题的广义解

研究了一类广义抛物型方程奇摄动问题.首先在一定的条件下, 提出了一类具有两参数的非线性非局部广义抛物型方程初始 边值问题.其次证明了相应问题解的存在性.然后, 通过Fredholm积分方程得到了初始 边值问题的外部解.再利用泛函分析理论和伸长变量及多重尺度法, 分别构造了初始 边值问题广义解的边界层、初始层项,从而得到了问题的形式渐近展开式.最后利用不动点理论证明了对应的非线性非局部广义抛物型方程的奇异摄动初始 边值问题的广义解的渐近展开式的一致有效性.     

Poincaré非线性振动理论在连续介质力学中的推广(Ⅱ)——若干应用

文本是文[1]的继续.文[1]中,提出和建议使用非线性偏微分方程直接摄动与加权积分方程法,计算连续介质系统的共振与非共振周期解.本文中,应用该方法计算了定跨度弹性梁在各种常见边界条件下强迫振动的共振与非共振周期解,方板在集中周期荷载作用下的共振周期解.指出了,非主振型对非线性振动周期解的影响及静荷载对幅频特性曲线的影响.     

一类广义非线性反应扩散方程奇摄动问题激波解（英文）

本文研究一类广义非线性反应扩散方程奇摄动初始边值问题.首先,构造非线性问题的外部解.其次,利用局部坐标系和伸长变量得到激波层和边界层校正项.最后,利用不动点理论研究了非线性反应扩散方程初始边值问题广义解的渐近性态.     

Lame equation and asymptotic higher-order periodic solutions to nonlinear evolution equations

Based on an auxiliary Lame equation and the perturbation method, a direct method is proposed to construct asymptotic higher-order periodic solutions to some nonlinear evolution equations. It is shown that some asymptotic higher-order periodic solutions to some nonlinear evolution equations in terms of Jacobi elliptic functions are explicitly obtained with the aid of symbolic computation.     

Computation of the normal forms for general M-DOF systems using multiple time scales. Part II: non-autonomous systems

A perturbation technique has been developed in Part I to consider the computation of the normal forms for general multiple-degree-of-freedom autonomous systems. In this paper, the perturbation approach is extended to study general non-autonomous systems and is focused on systems with external forcing. With the aid of multiple time scales, efficient recursive algorithms are developed for systematically computing the normal forms. General solutions are obtained for solving ordered perturbation equations. In particular, the following cases are considered in detail: the non-resonance, internal resonances (including general resonance, resonant case involving 1:1 primary resonance, and combination of resonant case with non-resonance), and external resonances (including general resonance, and combination of internal resonance and external resonance). User-friendly Maple programs have been coded which can be “automatically” executed on various computer systems. Examples are given to demonstrate the computational efficiency of the method and the convenience of using computer algebra systems.     

Perturbation Theory for the Solitary Wave Solutions to a Sasa‐Satsuma Model Describing Nonlinear Internal Waves in a Continuously Stratified Fluid

The adiabatic evolution of perturbed solitary wave solutions to an extended Sasa‐Satsuma (or vector‐valued modified Korteweg–de Vries) model governing nonlinear internal gravity propagation in a continuously stratified fluid is considered. The transport equations describing the evolution of the solitary wave parameters are determined by a direct multiple‐scale asymptotic expansion and independently by phase‐averaged conservation relations for an arbitrary perturbation. As an example, the adiabatic evolution associated with a dissipative perturbation is explicitly determined. Unlike the case with the dissipatively perturbed modified Korteweg–de Vries equation, the adiabatic asymptotic expansion for the Sasa‐Satsuma model considered here is not exponentially nonuniform and no shelf region emerges in the lee‐side of the propagating solitary wave.     

非线性扰动Klein-Gordon方程初值问题的渐近理论

在二维空间中研究一类非线性扰动Klein-Gordon方程初值问题解的渐近理论. 首先利用压缩映象原理,结合一些先验估计式及Bessel函数的收敛性,根据Klein-Gordon方程初值问题的等价积分方程,在二次连续可微空间中得到了初值问题解的适定性;其次,利用扰动方法构造了初值问题的形式近似解,并得到了该形式近似解的渐近合理性;最后给出了所得渐近理论的一个应用,用渐近近似定理分析了一个具体的非线性Klein-Gordon方程初值问题解的渐近近似程度．     

两自由度非线性振动系统主参数激励下的分岔分析

本文给出了参数激励作用下两自由度非线性振动系统,在1:2内共振条件下主参数激励低阶模态的非线性响应.采用多尺度法得到其振幅和相位的调制方程,分析发现平凡解通过树枝分岔产生耦合模态解,采用Melnikov方法研究全局分岔行为,确定了产生Smale马蹄型混沌的参数值.     

Stability analysis based on nonlinear inhomogeneous approximation

The asymptotic stability of zero solutions for essentially nonlinear systems of differential equations in triangular inhomogeneous approximation is studied. Conditions under which perturbations do not affect the asymptotic stability of the zero solution are determined by using the direct Lyapunov method. Stability criteria are stated in the form of inequalities between perturbation orders and the orders of homogeneity of functions involved in the nonlinear approximation system under consideration.     

一类催化反应Robin问题的渐近解

研究了一类非线性催化反应微分方程Robin问题.在一定的条件下,先利用摄动方法求出了原Robin问题的外部解,然后用伸长变量和幂级数理论分别构造了解的第一和第二边界层校正项,从而得到了Robin问题解的形式渐近展开式.最后利用微分不等式理论,证明了问题解的渐近表示式的一致有效性.     

Perturbations of Soliton Solutions to the Unstable Nonlinear Schrödinger and Sine-Gordon Equations

The adiabatic evolution of soliton solutions to the unstable nonlinear Schrödinger (UNS) and sine-Gordon (SG) equations in the presence of small perturbations is reconsidered. The transport equations describing the evolution of the solitary wave parameters are determined by a direct multiple-scale asymptotic expansion and by phase-averaged conservation relations for an arbitrary perturbation. The evolution associated with a dissipative perturbation is explicitly determined and the first-order perturbation fields are also obtained.     

On the Asymptotic and Numerical Analyses of Exponentially III-Conditioned Singularly Perturbed Boundary Value Problems

Asymptotic and numerical methods are used to study several classes of singularly perturbed boundary value problems for which the underlying homogeneous operators have exponentially small eigenvalues. Examples considered include the familiar boundary layer resonance problems and some extensions and certain linearized equations associated with metastable internal layer motion. For the boundary layer resonance problems, a systematic projection method, motivated by the work of De Groen [1], is used to analytically calculate high-order asymptotic solutions. This method justifies and extends some previous results obtained from the variational method of Grasman and Matkowsky [2]. A numerical approach, based on an integral equation formulation, is used to accurately compute boundary layer resonance solutions and their associated exponentially small eigenvalues. For various examples, the numerical results are shown to compare very favorably with two-term asymptotic results. Finally, some Sturm-Liouville operators with exponentially small spectral gap widths are studied. One such problem is applied to analyzing metastable internal layer motion for a certain forced Burgers equation.     

Global bifurcations of a taut string with 1:2 internal resonance

The global bifurcations of a taut string are investigated with the case of 1:2 internal resonance. The method of multiple scales is applied to obtain a system of autonomous ordinary differential equations. Based on the normal form theory, the desired form for the global perturbation method is obtained. Then the method developed by Kovacic and Wiggins is used to find explicit sufficient conditions for chaos to occur by identifying the existence of a Silnikov-type homoclinic orbit. Finally, numerical results obtained by using fourth-order Runge–Kutta method agree with the theoretical analysis at least qualitatively.