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An augmented formulation for mechanical systems with non-generalized coordinates: Application to rigid body contact problems

机译:具有非通用坐标的机械系统的增强公式:应用于刚体接触问题

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In computational multibody algorithms, the kinematic constraint equations that describe mechanical joints and specified motion trajectories must be satisfied at the position, velocity and acceleration levels. For most commonly used constraint equations, only first and second partial derivatives of position vectors with respect to the generalized coordinates are required in order to define the constraint Jacobian matrix and the first and second derivatives of the constraints with respect to time. When the kinematic and dynamic equations of the multibody systems are formulated in terms of a mixed set of generalized and non-generalized coordinates, higher partial derivatives with respect to these non-generalized coordinates are required, and the neglect of these derivatives can lead to significant errors. In this paper, the implementation of a contact model in general multibody algorithms is presented as an example of mechanical systems with non-generalized coordinates. The kinematic equations that describe the contact between two surfaces of two bodies in the multibody system are formulated in terms of the system generalized coordinates and the surface parameters. Each contact surface is defined using two independent parameters that completely define the tangent and normal vectors at an arbitrary point on the body surface. In the contact model developed in this study, the points of contact are searched for on line during the dynamic simulation by solving the nonlinear differential and algebraic equations of the constrained multibody system. It is demonstrated in this paper that in the case of a point contact and regular surfaces, there is only one independent generalized contact constraint force despite the fact that five constraint equations are used to enforce the contact conditions. [References: 19]
机译:在计算多体算法中,必须在位置,速度和加速度水平上满足描述机械关节和指定运动轨迹的运动约束方程。对于最常用的约束方程式,只需要相对于广义坐标的位置矢量的一阶和二阶导数即可定义约束雅可比矩阵,以及约束条件相对于时间的一阶和二阶。当根据广义坐标和非广义坐标的混合集来公式化多体系统的运动学和动力学方程时,相对于这些非广义坐标,需要更高的偏导数,而忽略这些导数可能会导致错误。本文以通用多体算法中的接触模型的实现为例,提出了具有非广义坐标的机械系统的示例。根据系统广义坐标和表面参数,制定了描述多体系统中两个物体的两个表面之间的接触的运动方程。每个接触表面使用两个独立的参数定义,这些参数完全定义了身体表面上任意点的切线和法线向量。在本研究开发的接触模型中,通过求解约束多体系统的非线性微分方程和代数方程,在动力学仿真过程中在线搜索接触点。本文证明,在点接触和规则曲面的情况下,尽管使用了五个约束方程式来强制执行接触条件,但只有一个独立的广义接触约束力。 [参考:19]

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