包含伺服约束的非完整系统的对称性摄动与绝热不变量

建立包含伺服约束系统的运动微分方程,基于包含伺服约束系统对称性与不变量理论研究包含伺服约束系统的对称性摄动与绝热不变量 问题,提出了包含伺服约束系统的高阶绝热不变量概念,证明了精确不变量与绝热不变量存在的条件及形式,并举例说明结果的应用。     

分数阶Birkhoff系统Noether对称性的摄动与绝热不变量

20世纪90年代以来,分数阶微积分理论与方法已被广泛地应用到自然科学和社会科学的各个领域,动力学与控制是其中的一个重要应用领域.为了进一步研究分数阶力学系统,本文基于Riemann-Liouville分数阶导数,讨论了分数阶Birkhoff系统Noether对称性的摄动与绝热不变量问题.首先,给出分数阶Birkhoff系统的运动微分方程及精确不变量;其次,给出绝热不变量的定义,并研究分数阶Birkhoff系统的绝热不变量;文末举例说明结果的应用.     

关于完整非保守系统的基本积分变量关系

本文证明,完整非保守系统不存在 Poincare-Cartan 积分不变量和 Poincare 通用积分不变量。取而代之,给出非保守系统的 Poincare-Cartan 型和 Poincare 型积分变量关系,并将这种积分变量关系用于求解非线性振动问题。我们还证明了文[1]、[2]所谓的积分不变量只是我们所引入的基本积分变量关系。     

Birkhoff系统的广义正则变换及其基本形式

动力学方程的积分问题是分析力学研究的一个重要方面．由于求解一般的动力学方程往往会遇到很大困难，因此可利用变量变换，使方程变得容易求解．文章研究Birkhoff系统的广义正则变换．首先，建立Birkhoff系统的广义正则变换的充分必要条件；其次，基于该条件，给出Birkhoff系统的广义正则变换的六种基本形式，导出每一种情况下新旧变量之间的变换关系．作为特例，文中给出Hamilton方程的正则变换．文末，给出算例以说明结果的应用．     

关于张量函数表示理论的标量不变量的讨论

发现文献[1,2]提出的张量函数表示理论中的完备而不可约的不变量不是互相完全独立的．分别对一个任意二阶张量和两个对称二阶张量的标量不变量进行了计算,证明前者只有六个不变量是独立的,后者只有九个是独立的．     

变质量非完整力学系统的Noether定理及其逆定理

1 引言动力学系统的守恒定律或运动积分是满足运动微分方程的物理量和几何量之间的某种确定的函数关系;动力学系统的对称性或不变性是指表征系统的某个特征对某个变换在某种意义下是不变的.1918年,A E Nocther 提出的Noether 定理,首先把动力学系统     

基于分数阶模型的非完整系统的Mei对称性及其守恒量

为了进一步揭示非完整系统的对称性和守恒量之间的内在关系，提出并研究基于分数阶模型的非完整系统的Mei对称性及其守恒量．首先，根据分数阶d’Alembert-Lagrange原理建立基于分数阶模型的非完整系统的动力学方程．其次，根据动力学方程中的动力学函数经无限小变换后仍满足原方程的不变性，建立分数阶模型下非完整系统的Mei对称性定理，给出Mei守恒量．再次，讨论了几个特例：分数阶Hamilton系统、经典非完整系统和受非完整约束的分数阶Lagrange系统的Mei对称性定理．文末举例说明结果的应用．     

非完整非保守系统在相空间的Noether定理及其逆定理

本文根据动力学系统在相空间的作用积分在无穷小群变换下的变换性质，得到了非完整非保守系统在相空间的Ｎｏｅｔｈｅｒ定理和逆定理。并举例说明。     

关于力学系统的对称性与不变量

本文综述了近10年来关于力学系统的对称性和不变量的研究所提出的新概念、新理论,主要包括经典Noether对称性的微分几何描述、高阶Noether对称性、Lie对称性,拟对称性和伴随对称性以及与之相应的不变量,关于非保守系统的高阶Noether对称性和Lie对称性的结果属首次公布。      

Birkhoff系统的一类积分不变量的构造

分别建立了自由Birkhoff系统和约束Birkhoff系统的非等时变分方程,并且利用系统的Birkhoff方程及其非等时变分方程证明,可由第一积分直接构造该系统基于非等时变分的一类积分不变量。文中,举例说明结果的应用。     

Constructing invariant tori for two weakly coupled van der Pol oscillators

An algorithm is developed for the construction of an invariant torus of a weakly coupled autonomous oscillator. The system is put into angular standard form. The determining equations are found by averaging and are solved for the approximate amplitudes of the torus. A perturbation series is then constructed about the approximate amplitudes with unknown coefficients as periodic functions of the angular variables. A sequence of solvable partial differential equations is developed for determining the coefficients. The algorithm is applied to a system of nonlinearly coupled van der Pol equations and the first order coefficients are generated in a straightforward manner. The approximation shows both good numerical accuracy and reproducibility of the periodicities of the van der Pol system. A comparitive analysis of integrating the van der Pol system with integrating the phase equations from the angular standard form on the approximate torus shows numerical errors of the order of the perturbation parameter =0.05 for integrations of up to 10,000 steps. Applying FFT to the numerical periodicities generated by integrating the van der Pol system near the tours reveals the same predominant frequencies found in the perturbation coefficients. Finally an expected rotation number is found by integrating the phase equations on the approximate torus.Contribution of the National Institute of Standards and Technology, a Federal agency.     

Adiabatic invariants for dynamical systems with one degree of freedom

Adiabatic invariants for dynamical systems with one degree of freedom, whose equation of motion is (1), and where the existence of the corresponding Hamilton action integral is not imposed, are established. The adiabatic invariants may vary according to their structure. Using the theory a few particular problems, including non-autonomous Duffing and Van der Pol oscillators, are analysed. Finally, it is indicated how the adiabatic invariants can be used for finding approximate solutions, stability analyses and for plotting phase curves.     

Perturbation to Noether symmetries and adiabatic invariants for disturbed Hamiltonian systems based on El-Nabulsi nonconservative dynamics model

This paper focuses on studying the perturbation to the Noether symmetries and the adiabatic invariants for nonconservative dynamic systems in phase space under nonconservative dynamics model presented by El-Nabulsi. First of all, the El-Nabulsi dynamics model for a nonconservative system is introduced and the El-Nabulsi–Hamilton canonical equations are established. Secondly, the basic formulae for the variation of El-Nabulsi–Hamilton action in phase space are deduced, the definition and criterion of the Noether quasi-symmetric transformation are given, and the exact invariant led directly by the Noether symmetry is obtained. Finally, based upon the concept of high-order adiabatic invariant of a mechanical system, the relationship between the perturbation to the Noether symmetry and the adiabatic invariant after the action of a small disturbance is studied and the conditions that the perturbation of symmetry leads to the adiabatic invariant and its formulation are given. At the end of the paper, two examples are given to illustrate the application of the method and results.     

Response analysis of fuzzy nonlinear dynamical systems

The transient and steady-state membership distribution functions (MDFs) of fuzzy response of a Duffing–Van der Pol oscillator with fuzzy uncertainty are studied by means of the fuzzy generalized cell mapping (FGCM) method. A rigorous mathematical foundation of the FGCM is established with a discrete representation of the fuzzy master equation for the possibility transition of continuous fuzzy processes. Fuzzy response is characterized by its topology in the state space and its possibility measure of MDFs. The evolutionary orientation of MDFs is in accordance with invariant manifolds toward invariant sets. In the evolutionary process of a steady-state fuzzy response with an increase of the intensity of fuzzy noise, a merging bifurcation is observed in a sudden change of MDFs from two sharp peaks of maximum possibility to one peak band around unstable manifolds.     

Response statistics of van der Pol oscillators excited by white noise

The joint probability density function of the state space vector of a white noise exoited van der Pol oscillator satisfics a Fokker-Planck-Kolmogorov (FPK) equation. The paper describes a numerical procedure for solving the transient FPK equation based on the path integral solution (PIS) technique. It is shown that by combining the PIS with a cubic B-spline interpolation method, numerical solution algorithms can be implemented giving solutions of the FPK equation that can be made accurate down to very low probability levels. The method is illustrated by application to two specific examples of a van der Pol oscillator.     

多尺度法二义性的一种解释

多尺度法是为解决含小参数系统发展起来的应用最广泛的摄动法之一. 在求解高阶近 似方程时,多尺度法一般只求特解. 用多尺度法求解van der Pol 方程的三阶解时 将出现矛盾. 以van der Pol方程为例,证明了忽略一阶修正量中的一阶谐波 项使得混合偏导数不能交换顺序,从而导致了多尺度法的二义性和另一个数学矛盾. 在求解一阶修正量时采用含有一阶谐波项的全解,消除了二义性和该矛盾. 该 方法所求得的近似解与数值解进行了比较,结果非常吻合,验证了其合理性.     

Orthogonal trajectories for nonlinear equations

Abdelkader developed a method for solving the van der Pol equation numerically. He observed that the orthogonal trajectories of the van der Pol equation satisfy a Riccati equation, the solution to which can be expressed in terms of Bessel functions. In the present paper, all nonlinear equations whose orthogonal trajectories satisfy Riccati or generalized Riccati equations are determined. Further on, another representation of the trajectories of the van der Pol equation is derived. This representation appears to be simpler than Abdelkader's.     

Fast parametrically excited van der Pol oscillator with time delay state feedback

We investigate the effect of a fast vertical parametric excitation on self-excited vibrations in a delayed van der Pol oscillator. We use the method of direct partition of motion to derive the main autonomous equation governing the slow dynamic in the vicinity of the trivial equilibrium. Then, we apply the multiple scales method on this slow dynamic to derive a second-order slow flow system describing the modulation of slow dynamic. In particular we analyze the slow flow to obtain the effect of a fast excitation on the regions in parameter space where self-excited vibrations can be eliminated. We have shown that in the case where the time delay and the feedback gains are imposed, fast vertical parametric excitation can be an alternative to suppress undesirable self-excited vibrations in a delayed van der Pol oscillator.     

Nonlinear dynamics and control of a variable order oscillator with application to the van der Pol equation

We investigate the dynamics and control of a nonlinear oscillator that is described mathematically by a Variable Order Differential Equation (VODE). The dynamic problem in question arises from the dynamical analysis of a variable viscoelasticity oscillator. The dynamics of the model and the behavior of the variable order differintegrals are shown in variable phase space for different parameters. Two different controllers are developed for the VODEs under study in order to track an arbitrary reference function. A generalization of the van der Pol equation using the VODE formulation is analyzed under the light of the methods introduced in this work.     

Van der Pol-Duffing方程的非线性动力学分叉特性研究

应用平均法研究Van der Pol-Duffing方程的幅频响应特性，并通过奇异性理论分析其静态分叉现象。进一步的动态分叉研究对系统参数空间进行了划分，发现在不同的参数区域内，系统相空间具有完全不同的拓扑特性，并应用胞映射方法分析了特定参数区域内的多吸引子共存现象。