耦合弹簧-摆系统的拉格朗日方程

Nur Widya Rini, Joko Saefan, Nur Khoiri
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引用次数: 0

摘要

研究了保守场中的耦合弹簧摆系统,利用拉格朗日方程和哈密顿方程得到了该系统的运动方程。运动方程由三个广义坐标的二阶微分方程表示。当系统处于平衡位置时,势能等于零。所采用的广义坐标为第一摆角θ_1,第二摆角θ_2,弹簧长度的增量x。由此得到的运动方程可用于确定系统在任何时刻的动力学行为。通过提供推导拉格朗日运动方程的程序,期望学生的理解更加完整。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Lagrangian Equation of Coupled Spring-Pendulum System
A coupled spring-pendulum system in a conservative field was studied where the equation of motion of the system using Lagrangian and Hamiltonian equation were obtained. The equation of motion represented by a second-order differential equation from the three generalized coordinate were used. The potential energy equal to zero when the system is in its equilibrium position. The generalized coordinate that being used were the angle of the first pendulum θ_1, the angle of the second pendulum θ_2, and the increase in the length of the spring x. The resulting equation of motion can be used to determine the dynamics behavior of the system at any time. Students' understanding is expected to be more complete by providing a procedure to derive the Lagrangian equation of motion.
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