非完整非保守系统的积分因子和守恒律

通过寻找积分因子来建立非完整非保守系统的守恒律，讨论了存在守恒定律的必要条件，并举例说明其应用。     

关于拉格朗日方程循环积分的讨论

作为《理论力学》课程的教学内容之一,教材中一般都给出了拉格朗日方程存在循环积分的充分条件.若拉格朗日函数中不显含某些广义坐标(称为循环坐标),则对于保守系统,对应于循环坐标的广义动量守恒.给出了非保守动力学系统的拉格朗日方程存在循环积分的条件,并用教材中常用的算例讨论了广义动量守恒的物理含义.结果表明用拉格朗日方程的循环积分比用动量定理和动量矩定理更容易找到系统的守恒量.     

分数阶拟周期Mathieu方程的动力学分析

分数阶微积分有着诸多优异的特点, 目前在动力学领域主要用来提高非线性系统振动特性研究的准确性. 本文在拟周期Mathieu方程的基础上, 引入分数阶微积分理论, 研究了分数阶微分项参数对方程稳定性的影响. 首先, 采用摄动法得到方程稳定区和非稳定区分界线(即过渡曲线)近似表达式, 利用数值方法验证了解析结果的准确性, 图像显示两者吻合较好. 随后, 通过归纳总结不同情况下的过渡曲线近似表达式, 发现在系统中分数阶微分项以等效线性刚度和等效线性阻尼的方式存在. 根据这一特点, 得到了系统等效线性阻尼和等效线性刚度的一般形式, 并且定义了非稳定区域厚度. 最后, 通过数值仿真直观地分析了分数阶微分项参数对方程稳定区域大小和过渡曲线位置的影响. 结果发现, 分数阶微分项不仅具有阻尼特性还具有刚度特性, 并且以等效线性刚度和等效线性阻尼的方式影响着方程稳定区域大小和过渡曲线位置. 合理选择分数阶微分项参数可以使其呈现不同程度的刚度特性或阻尼特性, 方程稳定区域的大小和过渡曲线的位置也因此产生了不同程度的变化.      

完整力学系统的共形不变性与守恒量

将Birkhoff方程的共形不变性和共形因子的概念拓展到完整力学系统,研究一般完整力学系统在无限小变换下的共形不变性与守恒量.给出了一般完整力学系统的共形不变性的定义和确定方程;研究了系统的Noether对称性与共形不变性之间的关系,研究表明,当Noether对称变换的生成元和非势广义力满足一定条件时,变换也是共形不变的,给出了相应的共形因子表达式,得到了一般完整力学系统的共形不变性直接导致的Noether守恒量;研究了系统的Lie对称性与共形不变性之间的关系,给出了与Lie对称性相应的无限小变换共形不变的充分必要条件,得到了一般完整力学系统的共形不变性直接导致的Lutzky守恒量.文中还举例说明结果的应用.     

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.     

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．     

受匀速转动约束的变质量非完整力学系统的Appell方程

本文建立受匀速转动约束的变质量非完整力学系统l...     

一种基于微分求积的空间分数阶扩散方程求解方法

通过微分求积建立求解变系数空间分数阶扩散方程的一种有效直接数值方法.基于Reciprocal Mul-tiquadric和Thin-Plate Spline径向基函数推导两种逼近分数阶导数的微分求积公式,将所考虑的模型问题转化成易求解的常微分方程组,并采用Crank-Nicolson格式进行离散.给出5个数值算例,计算...     

任意阶非完整约束系统的Appell型方程

本文从万有D'Alembert原理出发,得到任意阶非完整约束系统的Appell型方程,在此基础上可给出本结果的推论.     

任意阶非完整约束系统的Appell型方程

本文从万有D'Alembert原理出发,得到任意阶非完整约束系统的Appell型方程,在此基础上可给出本结果的推论.     

具有稳定数值解的三维谐振子

谐振子广泛应用于物理系统的描述和物理现象的数值模拟.由于二维或三维谐振子对于系统参数、初始条件和边界条件的高度敏感性,很多物理过程的动力学模拟都会出现数值解不稳定的现象.近年来发展的无网格法、物质点法和近场动力学法等数值模拟方法均绕开了对固体材料固有构形的量化描述.本文引入了定常耗散项和弹簧耗散项,考虑随机微扰效应,提...     

Integral invariants of a holonomic dynamical ststem

ＩＮＴＥＧＲＡＬＩＮＶＡＲＩＡＮＴＳＯＦＡＨＯＬＯＮＯＭＩＣＤＹＮＡＭＩＣＡＬＳＴＳＴＥＭＮａｓｅｅｒＡｈｍｅｄ（ＭａｔｈｅｍａｔｉｃｓＤｅｐａｒｔｍｅｎｔ．Ｑｕａｉｄ－ｉ－ＡｚａｍＵｎｉｖｅｒｓｉｔｙ,Ｉｓｌａｍａｂａｄ,Ｐａｋｉｓｔａｎ）（Ｒｅｃ...     

Attractors of Parabolic Equations Without Uniqueness

In this paper we study the existence of global compact attractors for nonlinear parabolic equations of the reaction-diffusion type and variational inequalities. The studied equations are generated by a difference of subdifferential maps and are not assumed to have a unique solution for each initial state. Applications are given to inclusions modeling combustion in porous media and processes of transmission of electrical impulses in nerve axons.     

Singularity-free augmented Lagrangian algorithms for constrained multibody dynamics

After a general review of the methods currently available for the dynamics of constrained multibody systems in the context of numerical efficiency and ability to solve the differential equations of motion in singular positions, we examine the acceleration based augmented Lagrangian formulations, and propose a new one for holonomic and non-holonomic systems that is based on the canonical equations of Hamilton. This new one proves to be more stable and accurate that the acceleration based counterpart under repetitive singular positions. The proposed algorithms are numerically efficient, can use standard conditionally stable numerical integrators and do not fail in singular positions, as the classical formulations do. The reason for the numerical efficiency and better behavior under singularities relies on the fact that the leading matrix of the resultant system of ODEs is sparse, symmetric, positive definite, and its rank is independent of that of the Jacobian of the constraint equations. The latter fact makes the proposed method particularly suitable for singular configurations.     

Numerical simulation of nonholonomic rigid-body systems

The paper proposes computer algebra system (CAS) algorithms for computer-assisted derivation of the equations of motion for systems of rigid bodies with holonomic and nonholonomic constraints that are linear with respect to the generalized velocities. The main advantages of using the D’Alembert-Lagrange principle for the CSA-based derivation of the equations of motion for nonholonomic systems of rigid bodies are demonstrated. Among them are universality, algorithmizability, computational efficiency, and simplicity of deriving equations for holonomic and nonholonomic systems in terms of generalized coordinates or pseudo-velocities __________ Translated from Prikladnaya Mekhanika, Vol. 42, No. 9, pp. 106–115, September 2006.     

Canonical forms of Nielsen's and Cenov's dynamical equations

In this paper, with Poincaré's formalism, and an indirect method, the canonical forms of the generalized equations of motion due to Nielsen and Cenov of a holonomic dynamical system in the velocity-phase space and the acceleration-phase space are obtained in terms of the Poincaré parameters This paper was presented at the International Congress of Mathematicians (ICM), 21–29 August, 1990, Kyoto University, Japan.     

Exponential Attractors in Banach Spaces

In this paper we extend the theory of exponential attractors from the Hilbert space setting in [4] to the Banach space setting. No squeezing conditions are needed; the only requirements are for the semiflow to be C ¹ in some absorbing ball, and for the linearized semiflow at every point inside the absorbing ball to split into the sum of a compact operator plus a contraction.