用摄动分析连续陀螺系统的稳定性

R. Parker
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摘要

连续陀螺系统的特征值和稳定性只能在有限的情况下解析计算。本文提出了一种特征值摄动分析方法,以确定临界速度和零速度附近的近似特征值轨迹和稳定性结论。摄动分析依赖于一般连续陀螺仪系统特征值问题的矩阵微分算子和向量特征函数的表述。特征值λ在公式中仅以λ2的形式出现,λ2在临界速度和零速度下的平滑性是摄动所需的基本特征。在临界速度和零速度下确定了一阶特征值摄动。导出的特征值摄动是原始质量、陀螺仪和刚度算符以及临界速度/静止系统特征函数的简单表达式。预测一个特征值是否进入或离开一个散度不稳定区域是由特征值扰动的符号决定的。此外,临界速度/静止系统的扰动产生了远离这些速度的特征值轨迹的近似值。结果为估计连续陀螺系统的特征值和临界速度附近的稳定性提供了一种无需数值计算的解析方法。结果仅限于具有与每个临界速度和每个平稳系统特征值相关的一个独立特征函数的系统。这些技术也适用于离散陀螺仪系统。给出了轴向运动受拉梁和旋转刚体的算例,并与已知解进行了比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Stability of Continuous Gyroscopic Systems Using Perturbation Analysis
Continuous gyroscopic system eigenvalues and stability are analytically calculable in only a limited set of cases. This paper presents an eigenvalue perturbation analysis to determine approximate eigenvalue loci and stability conclusions in the vicinity of critical speeds and zero speed. The perturbation analysis relies on a formulation of the general continuous gyroscopic system eigenvalue problem in terms of matrix differential operators and vector eigenfunctions. The eigenvalue λ appears only as λ2 in the formulation, and the smoothness of λ2 at the critical speeds and zero speed is the essential feature required for the perturbatton. First order eigenvalue perturbations are determined at the critical speeds and zero speed. The derived eigenvalue perturbations are simple expressions in terms of the original mass, gyroscopic, and stiffness operators and the critical speed/stationary system eigenfunctions. Prediction of whether an eigenvalue passes to or from a region of divergence instability is determined by the sign of the eigenvalue perturbation. Additionally, perturbation of the critical speed/stationary system yields approximations for the eigenvalue loci at speeds away from these. The results provide analytical means for estimating continuous gyroscopic system eigenvalues and stability near critical speeds without numerical computation. The results are limited to systems having one independent eigenfunction associated with each critical speed and each stationary system eigenvalue. The techniques also apply to discrete gyroscopic systems. Examples are presented for an axially-moving, tensioned beam and a rotating rigid body and comparisons with known solutions are given.
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