非保守弹性动力学初值问题的简单Gurtin型拟变分原理

按照广义力和广义位移之间的对应关系,将弹性动力学基本方程卷积乘上相应的虚量,然后积分且代数相加,并利用体积力和面积力均为伴生力这一特征,建立了非保守系统初值问题的简单Gurtin型五类变量的完全拟变分原理.更进一步地还建立了非保守系统初值问题的简单Gurtin型不完全拟变分原理和有条件不完全拟变分原理.在建立非保守系统初值问题的各类简单Gurtin型拟变分原理的同时,还将变积方法推广为卷变积方法.最后,介绍了寻求伴生力的方法.     

变质量非完整系统相对运动动力学方程的积分理论

本文研究变质量非线性非完整系统相对于非惯性系动力学的积分理论，给出其Ｒｏｕｔｈ降阶法，Ｗｈｉｔｔａｋｅｒ降阶法，Ｐｏｉｎｃａｒｅ－Ｃａｒｔａｎ型积分变量关系和积分不变量。     

非保守系统的有限变形弹性变分原理

最近,文献[1]将小变形弹性理论中关于保守系统的变分原理向非保守系统作了推广,其出发点是小变形弹性理论中的两个最小值原理.由于所建立的变分原理只能以变分式的形式出现,故称之为拟变分原理。本文直接从有限变形弹性理论的虚功原理出发,建立非保守系统的有限变形弹性拟变分原理.与文献[1]相比,我们的推广不仅在内容上更为一般,而且方法更为直接、简单.     

分数因子与分数阶完整力学系统的运动方程和循环积分

引入分数因子和分数增量,给出了分数阶微积分的定义和性质;基于分数阶导数的定义,证明了含有分数因子的等时变分与分数阶算子的交换关系;提出了分数阶完整保守和非保守系统的Hamilton原理;建立了分数阶完整保守系统和非保守系统的运动微分方程;得到了分数阶完整保守系统的循环积分;并利用分数阶循环积分导出分数阶罗兹方程．最后给出了两个例子．研究表明利用分数因子给出的分数阶微分方程是一个含有分数因子的通常的微分方程,那么分数阶系统运动微分方程的求解都可以采用通常微分方程的求解方法．     

关于线粘弹性动力学中各种变分原理

本文提出一条简单而统一的新途径,系统地建立了线粘弹性动力学中各种简化Gurtin型变分原理,文中首先给出一个很有用的以卷积表示的积分关系式,然后从该式出发,系统地导出成互补关系的五类变量、四类变量、三类变量、二类变量及一类变量简化Gurtin型变分原理,并清楚地阐明它们之间的内在联系,而且,还发现当前在国际上有广泛影响的力学变分原理方面的名著[1]及文[2]中,所给出的四个变分原理的泛函式均有误.本文除给出这四个正确的泛函式外,还建立了一些新的更一般广义变分原理。     

弹性非保守系统的拟固有频率变分原理及其应用

本文在文献[1]的基础上,进一步考虑系统的运动性态,提出并证明了弹性非保守系统自激振动的拟固有频率变分原理,然后利用这些变分原理计算了几个典型的非保守系统的稳定性问题.结果表明本文提出的变分原理不仅是分析非保守系统颤振问题的一个强有力的工具,而且还为建立一些近似方法提供了理论依据.     

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。     

有限元法的基础——变分原理在非保守问题中的应用

对非保守机械系统,传统的哈密顿变分原理不能认为是正确的。因此,对那种类型的系统,有限元法的一个合适基础似乎不存在.本文将指出用另一个适当的泛函代替啥密顿的时间积分以及用一个拟标量积代替标量积,可以建立一个适当的函数空间,在那个函数空间中,传统的非保守系统——即关于能量是非保守的系统具有保守系统的性质。尤其是,在新的函数空间中,可以类似于哈密顿原理建立起变分原理。所以,有限元法用于非保守机械系统如同在通常的保守系统的应用一样地方便。最后用跟随力(follower forces)的非保守系统来说明这个理论.     

非完整系统正则形式的ЧАПЛЫТИН方程的一种降阶方法

文中根据能量积分进一步研究了非完整系统正则形式的ЧАПЛЫГИН方程的降阶问题,得到了处理这类系统的一般积分方法.给出的两个例子表明,该方法比文[3,4]更具优越性.     

非完整系统的Lie对称性与Noether对称性

研究非完整系统的Lie对称性与Noether对称性及其间的关系,具体研究了Chetaev型变量质量非完整系统和非Chetaev型非完整系统的Lie对称性与Noether对称性。给出Lie对称性导致Noether对称性及Noether对称性导致Lie对称性的条件。     

About the basic integral variants of holonomic nonconservative dynamical systems

In this paper, we prove that for holonomic nonconservative dynamical system the Poincaré and Poincaré-Cartan integral invariants do not exist. Instead of them, we introduce the integral variants of Poincaré-Cartan's type and of Poincare's type for holonomic nonconservative dynamical systems, and use these variants to solve the problem of nonlinear vibration. We also prove that the integral invariants introduced in references [1] and [2] are merely the basic integral variants given by this paper. Project supported by National Natural Science Foundation of China     

Conservation laws of dynamical systems via d'alembert's principle

In this note we study a method for finding the conserved quantities of nonconservative holonomic dynamical systems. In contrast to the classical Noetherian approach, which is based upon the variational principle of Hamilton, the starting point in this note is based on the differential principle of D'Alembert which is equally valid for conservative and nonconservative systems. In the second part of this note, an attempt is made to employ symmetry properties as a vehicle for obtaining approximate solutions of linear and non-linear dynamical systems.     

Noether's conservation laws of holonomic nonconservative dynamical systems in generalized mechanics

In the present paper, three kinds of forms for Noether's conservation laws of holonomic nonconservative dynamical systems in generalized mechanics are given. First Received Dec. 4, 1992     

A field method for solving the equations of motion of nonholonomic systems

In this paper, the field method^[1] for solving the equations of motion of holonomic nonconservative systems is extended to nonholonomic systems with constant mass and with variable mass. Two examples are given to illustrate its application. The project supported by the National Natural Science Foundation of China.     

Characterization of Measures Satisfying the Pesin Entropy Formula for Random Dynamical Systems

In this paper we first give a formulation of SRB (Sinai–Ruelle–Bowen) property for invariant measures of stationary random dynamical systems and then prove that this property is sufficient and necessary for a formula of Pesin's type relating entropy and Lyapunov exponents of such dynamical systems. This result is a random version of the main result in Part I of Ledrappier and Young's celebrated paper [11].     

INTEGRAL INVARIANT IN NONCONSERVATIVE SYSTEMS AND ITS APPLICATION IN MODERN PHYSICS

In this paper,the Poincaré and Poincaré-Cartan integral invariants in nonconservativesystems are established.According to the integral invariant,he non-linear oscillation ofparticles in 3-folded symmetry spiral sector cyclotron is investigated.It turns out that themethod is successful.     

Extension of Whittaker equations to non-holonomic mechanical systems

In 1904, using the energy integral Whittaker studied the reduction of a dynamical problem to a problem with fewer degrees of freedom for the holonomic conservative systems and obtained the Whittaker equation^[1].In this article, Whittaker equations are extended to non-holonomic systems and the generalized Whittaker equations are obtained. And then these equations are transformed into Kiel-sen’s form.Finally an example is given.     

Continuity of Dynamical Structures for Nonautonomous Evolution Equations Under Singular Perturbations

In this paper we study the continuity of invariant sets for nonautonomous infinite-dimensional dynamical systems under singular perturbations. We extend the existing results on lower-semicontinuity of attractors of autonomous and nonautonomous dynamical systems. This is accomplished through a detailed analysis of the structure of the invariant sets and its behavior under perturbation. We prove that a bounded hyperbolic global solutions persists under singular perturbations and that their nonlinear unstable manifold behave continuously. To accomplish this, we need to establish results on roughness of exponential dichotomies under these singular perturbations. Our results imply that, if the limiting pullback attractor of a nonautonomous dynamical system is the closure of a countable union of unstable manifolds of global bounded hyperbolic solutions, then it behaves continuously (upper and lower) under singular perturbations.