摘要
多体系统中柔性体运动一般分为体参考系的范围运动和变形运动。在多数场合,柔性体的变形运动是较小的,可以用对变形广义坐标线性化的动力学方程描述系统动力学行为。但是,目前通用的一些动力学建模方法用于柔性体动力学建模时,存在过早线性化缺陷,导致最终的动力学方程遗失了一些重要的刚柔耦合项。本文采用非线性变形场描述,计及含有变形广义坐标及其导数的二阶小量项,将这种非线性保留到求出偏(角)速度后,再线性化,建立了柔性多体系统相邻柔性体之间参考坐标系的运动学关系,为进一步建立系统动力学方程提供了理论基础。
The motion of flexible bodies in a multibody system can be represented in manyapplications as a superposition of a large references and small deformations,which allows linearization form of the deformation varianles in the dgnamic eqwations.But the defaults exist in some presesnt modeling methods,which are premature lineareization to the deformation variables,and result from rigid-flexible coupling terms losing in final dynamic equations. In this paper,a deformation field of a body is described by using second non-linear of deformation vaiables,and motion variables ane linearized after parial (angular)velocities are obtained. Kinematic relations between coordinate refevences of two adjecent bodies are develoed,which provides the theortical basis for dynamic modeling of flexible multibody systems.
出处
《河北工业大学学报》
CAS
1998年第4期1-7,共7页
Journal of Hebei University of Technology
基金
中国航天总公司博士后科学基金
河北省教委博士启动资金
国家航天863高技术项目基金
关键词
柔性多体系统
动力学
运动学
多体系统
变形
Flexible multibody system,Consistence liearizaion dynamic equation,Rigid-flexible coupling,Dynamics