相空间中有二阶线性单面约束的非完整系统的Lie对称性与守恒量

研究相空间中有二阶线性单面约束的非完整系统的Lie对称性与守恒量。首先根据微分方程在无限小变换下的不变性建立Lie对称性所满足的确定方程和限制方程，给出结构方程和守恒量；其次讨论系统的Lie对称性逆问题。最后举一实例说明结果的应用。     

事件空间中Herglotz型非保守Lagrange系统的Noether定理

研究事件空间中Herglotz型非保守Lagrange系统的Noether定理．首先,将Herglotz广义变分原理推广到事件空间,并基于该原理导出事件空间中Herglotz型Lagrange方程;其次,引入无限小变换,研究HamiltonHerglotz作用量的不变性,建立事件空间中Herglotz型Noether对称性的定义,并给出其判据方程;第三,提出并证明事件空间中Herglotz型Noether定理和Noether逆定理．最后,以Emden方程和黏性阻尼振子为例介绍Herglotz型Noether定理的应用．     

单面约束系统动力学研究进展

综述了单面约束系统动力学研究的历史与现状，并提出未来研究的建议。     

具有单面非线性非完整约束的动力学系统的运动

本文提出并研究了具有单面非线性非完整约束的动力学系统的运动问题,给出了描述系统运动的Ｂｏｌｔｚｍａｎｎ－Ｈａｍｅｌ型方程,并举例说明结果的应用。     

建立多自由度系统动力学方程的矩阵递推方法

本文采用了微分几何原理,运用法空间与切空间的正交性,采用逐次施加约束的方法,实现了受约束系统的降维,并得到了最终的动力学方程。     

虚功原理的一个推广形式

通常的虚功原理是在"理想、双面、稳定约束"的前提下来讨论体系平衡的充分必要条件的。这使得它不能直接用于含有单面约束的体系。本文将给出虚功原理的一个推广形式,用这一推广形式,将可以讨论某些含有单面约束的体系的平衡条件。为给出这一推广形式,我们先引入几个概念。设一体系存在若干约束(可以是双面的,也可以有 ...     

THE GENERALITY OF THE GENERAL EQUATIONS OF DYNAMICS 1)

理论力学中动力学普遍方程,在分析力学中称为d'Alembert--Lagrange原理。动力学普遍方程之普遍在于,由它不仅可导出动力学普遍定理,可导出完整约束系统和非完整约束系统的运动微分方程,还可导出积分变分原理。     

动力学普遍方程的普遍性——分析力学札记之三十一

理论力学中动力学普遍方程,在分析力学中称为d’Alembert–Lagrange原理。动力学普遍方程之普遍在于,由它不仅可导出动力学普遍定理,可导出完整约束系统和非完整约束系统的运动微分方程,还可导出积分变分原理。     

约束多体系统动力学的局部子空间分解法

由约束矩阵及其正交补的列矢量张成约束多体系统的局部约束子空间和局部切向子空间．将系统的广义加速度和广义力沿这两个子空间分解，推导描述系统运动的纯微分方程和求约束反力的公式，并给出了违约修正的一种有效方法     

经典力学基本微分原理与不完整力学组的运动方程

本文引入坐标空间、速度空间和加速度空间三个基本空间概念,给出了各个空间所对应的约束和虚位移的定义.以此作为基础,对经典力学的三个基本微分原理(D'Alembert-Lagrange原理,Bertrand原理以及Gauss原理)给出了统一的表述.此外,又从Bertrand原理出发,导出了关于不完整力学组的一系列运动方程.     

相空间中非保守系统的Herglotz广义变分原理及其Noether定理

与经典变分原理相比,基于由微分方程定义的作用量的Herglotz广义变分原理给出了非保守动力学系统的一个变分描述,它不仅能够描述所有采用经典变分原理能够描述的动力学过程,而且能够应用于经典变分原理不能适用的非保守或耗散系统.将Herglotz广义变分原理拓展到相空间,研究相空间中非保守力学系统的Herglotz广义变分原理与Noether定理及其逆定理.首先,提出相空间中Herglotz广义变分原理,给出相空间中非保守系统的变分描述,导出相应的Hamilton正则方程;其次,基于非等时变分与等时变分之间的关系,导出相空间中Hamilton-Herglotz作用量变分的两个基本公式;再次,给出Noether对称变换的定义和判据,提出并证明相空间中非保守系统基于Herglotz变分问题的Noether定理及其逆定理,揭示了相空间中力学系统的Noether对称性与守恒量之间的内在联系.在经典条件下,Herglotz广义变分原理退化为经典变分原理,与之相应的相空间中的Noether定理退化为经典Hamilton系统的Noether定理.文末以著名的Emden方程和平方阻尼振子为例说明上述方法和结果的有效性.     

时间尺度上Herglotz变分原理及其Noether定理

Herglotz变分原理的作用量是由微分方程定义的,不仅可以描述所有经典变分原理能够描述的动力学过程,还可以对经典变分原理不能适用的非保守系统或耗散系统进行变分描述．时间尺度上微积分理论提供了一种可同时研究离散系统和连续系统的有效方法．本文结合Herglotz变分原理和时间尺度微积分理论来研究时间尺度上的Herglotz变分原理及其Noether定理．首先,给出时间尺度上Lagrange系统的Herglotz变分原理．其次,根据Herglotz变分原理和Dubois-Reymond引理,推导出时间尺度上Lagrange系统的Herglotz变分问题的运动微分方程．再次,基于时间尺度上Hamilton-Herglotz作用量在群的无限小变换下的不变性,给出Noether对称性的定义并导出其Noether等式．最后,建立了时间尺度上Lagrange系统的Herglotz变分问题的Noether定理,给出了连续和离散两种情况下基于Herglotz变分问题的Noether守恒量．文末举例说明结果的应用．     

Noether's theorem for nonholonomic systems of non-Chetaev's type with unilateral constraints in event space

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Extended constraint enforcement formulations for finite-DOF systems based on Gauss’s principle of least constraint

Nonlinear Dynamics - This paper aims to contribute to formulations of mathematical models for finite-DOF systems based on the Gauss’s principle of least constraint. A new theorem allows to...     

Stability properties of equilibrium sets of non-linear mechanical systems with dry friction and impact

In this paper, we will give conditions under which the equilibrium set of multi-degree-of-freedom non-linear mechanical systems with an arbitrary number of frictional unilateral constraints is attractive. The theorems for attractivity are proved by using the framework of measure differential inclusions together with a Lyapunov-type stability analysis and a generalisation of LaSalle’s invariance principle for non-smooth systems. The special structure of mechanical multi-body systems allows for a natural Lyapunov function and an elegant derivation of the proof. Moreover, an instability theorem for assessing the instability of equilibrium sets of non-linear mechanical systems with frictional bilateral constraints is formulated. These results are illustrated by means of examples with both unilateral and bilateral frictional constraints.     

On the kinematic minimum principle for the rate problem in classical plasticity

An alternative form is given of the kinematic minimum principle for the rate problem in classical, small displacement plasticity. This study was motivated by the theorem given by G. Maier (1969) based on a quadratic programming approach, but the result is derived from the classical theorem and has a simpler form than Maier's theorem.     

Eigenvalue-counting methods for non-proportionally damped systems

This paper presents numerical methods of counting the number of eigenvalues for non-proportionally damped system in some interested regions on the complex plane. Most of the eigenvalue analysis methods for proportionally damped systems use the well-known Sturm sequence property to check the missed eigenvalues when only a set of the lowest modes is used. However, in the case of the non-proportionally damped systems such as the soil–structure interaction system, the structural control system and composite structures, no counterpart of the Sturm sequence property for undamped systems has been established yet. In this study, a numerical method based on argument principle is explained with emphasis on the discretization of the contour and a new method based on Gleyse’s theorem is proposed. To verify the applicability of the methods, two numerical examples are considered.     

THE THEOREM OF THE STABILITY OF NONLINEAR NONAUTONOMOUS SYSTEMS UNDER THE FREQUENTLY-ACTING PERTURBATION—LIAPUNOV’S INDIRECT METHOD

In this paper the stability of nonlinear nonautonomous systems under the frequently-acting perturbation is studied. This study is a forward development of the study of the stability in the Liapunov sense; furthermore, it is of significance in practice since perturbations are often not single in the time domain. Malkin proved a general theorem about thesubject. To apply the theorem, however, the user has to construct a Liapunov function which satisfies specified conditions and it is difficult to find such a function for nonlinear nonautonomous systems. In the light of the principle of Liapunov’s indirect method, which is an effective method to decide the stability of nonlinear systems in the Liapunov sense, the authors have achieved several important conclusions expressed in the form of theorems to determine the stability of nonlinear nonautonomous systems under the frequently-acting perturbation.     

Some Theorems in the Theory of Microstretch Thermomagnetoelectroelasticity

The linear dynamic theory of microstretch thermomagnetoelectroelasticity is studied in this paper.First,a reciprocity relation which involves two processes at different instants is established to form the basis of a uniqueness result and a reciprocal theorem.The proof of the reciprocal theorem avoids both using the Laplace transform and incorporating the initial conditions into the equations of motion.The uniqueness theorem is derived with no definiteness assumption on the elastic constitutive coefficients.Then the continuous dependence theorem is discussed upon two external data systems.Finally,the variational principle of Hamilton type which fully characterizes the solution of the mixed boundary-initial-value problem(mixed problem) is obtained.These theorems lay a solid foundation for further theoretical and numerical studies on microstretch thermomagnetoelectroelastic materials.     

THE THEOREM OF THE STABILITY OF NONLINEAR NONAUTONOMOUS SYSTEMS UNDER THE FREQUENTLY-ACTING PERTURBATION—LIAPUNOV’S INDIRECT METHOD

In this paper the stability of nonlinear nonautonomous systems under the frequently-acting perturbation is studied.This study is a forward development of the study of thestability in the Liapunov sense;furthermore,it is of significance in practice sinceperturbations are often not single in the time domain.Malk in proved a general theoremabout thesubject.To apply the theorem,however,the user has to construct a Liapunovfunction which satisfies specified conditions and it is difficult to find such a function fornonlinear nonautonomous systems.In the light of the principle of Liapunov’s indirectmethod,which is an effective method to decide the stability of nonlinear systems in theLiapunov sense,the authors have achieved several important conclusions expressed in theform of theorems to determine the stability of nonlinear nonautonomous systems under thefrequently-acting perturbation.