圆柱坐标系下基于Maple的非完整约束动力学对象建模RÃ-S ^ 1Ã-SO (3)

M. Ariska, H. Akhsan, M. Muslim, J. Pebralia, A. R. Sinensis, T. Aprianti
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引用次数: 0

摘要

动态系统的可靠实时规划在当今快速增长的自动化生态系统中至关重要,例如规划机器人系统的环境和方法。本文描述了在RÃ-S ^ 1Ã-SO (3)Â位形空间上具有非完整约束的刚体动力学系统。所采用的方法是运动规划网络和物理计算的数值处理,可用于非完整物体系统的实时运动,采用Jellets invariarian (JI)方法。该方法可以得到运动系统方程,并对具有非完整约束的目标模型进行评估,还可以显示在the RÃ-S ^ 1Ã-SO (3)Â位形空间中导航的实验结果。所使用的非完整约束运动系统是Tippe top (TT)。TT是一种像陀螺一样的玩具,当旋转时,它会用它的杆翻转自己。作者已经完成了在the Â位形空间中用各种坐标描述初始状态的TT运动的实时动力学模拟。根据前人对类似物体的研究结果,采用Eular-Lagrange方程、Routhian约化方程和Poincare方程求解TT。作者成功地描述了在the R^ 2Ã-SO (3)Â位形空间中具有预定初始条件和各种坐标的TT运动动力学。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Modeling of Dynamics Object with Non-Holonomic Constraints Based on Maple in Cylinder Coordinate R×S^1×SO(3)
Reliable real-time planning for dynamic systems is crucial in today's rapidly growing automated ecosystem, such as the environment and methods of planning a robotic system. This paper describes the rigid dynamics system with non-holonomic constraints on the R×S^1×SO(3) configuration space. The method used is the motion planning network and numeric treatment using physics computation which can be used for non-holonomic object systems that move in real-time with Jellets Invarian (JI) approach. The JI approach can result in a motion system equation and evaluate the model of an object with non-holonomic constraints and also display experimental results for navigation in the R×S^1×SO(3)  configuration space. The motion system with non-holonomic constraints used is Tippe top (TT). TT is a toy like a top which when rotated will flip itself with its stem. The author have finished in simulating the dynamics of TT motions in real time with the initial states that have been described with various coordinate in the   configuration space. Based on the results of previous studies on similar objects, TT was solved by the Eular-Lagrange Equation, Routhian Reduction Equation and Poincare. The author succeeded in describing the dynamics of TT motion in real time with predetermined initial conditions with various coordinates in the  R^2×SO(3) configuration space.
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