带流体动力轴承的转盘/主轴系统的自由振动

T. Jintanawan, I. Shen
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引用次数: 2

摘要

本文研究了带动液轴承的转盘/主轴系统的自由振动问题。盘/主轴系统由夹紧在刚性主轴上的多个圆盘组成,允许无限小的刚体平移和旋转(摇摆)。此外,主轴通过两个相同的径向组板和推力组板安装在固定的、灵活的悬臂轴上。首先推导了主轴刚体平移和摇摆、轴弯曲和盘振动的运动方程。然后进行特征值分析,得到旋转盘/主轴系统的固有频率、模态阻尼因子和模态振型。对于刚性轴和解耦平移/摇摆主轴的特殊情况,观察到一对横向模态和两对摇摆模态。对于横向模式,圆盘/主轴系统作为刚体以一半转速(即半速旋转)横向旋转。此外,向后旋转的阻尼很大,而向前旋转的阻尼很小。第一对摇摆模式类似于那些发现在圆盘/主轴系统与球轴承和轻微阻尼。第二对摇摆模式发生在低频。其中一种模式是轻微阻尼的,其固有频率非常接近转速的一半。对于柔性轴和耦合平移/摇摆运动的一般情况,得到了八种耦合模态。其中三个发生在半速频率。与刚性轴系统相比,由于轴的柔性,其他五种模态的固有频率明显降低。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Free Vibration of a Rotating Disk/Spindle System With Hydrodynamic Bearings
This paper is to study free vibration of a rotating disk/spindle system with hydrodynamic bearings (HDB). The disk/spindle system consists of multiple circular disks clamped on a rigid spindle, which allows infinitesimal rigid-body translation and rotation (rocking). Also, the spindle is mounted on a stationary, flexible, cantilever shaft through two identical radial HDB and a thrust HDB. Equations of motion were first derived in terms of the rigid-body translation and rocking of the spindle, the shaft bending, and the disk vibration. Then an eigenvalue analysis was performed to obtain natural frequencies, modal damping factors, and mode shapes of the rotating disk/spindle system. For a special case of rigid shaft and decoupled translation/rocking spindle, one pair of transverse modes and two pairs of rocking modes were observed. For the transverse modes, the disk/spindle system whirls transversely as a rigid body at half of the rotational speed (i.e., half-speed whirl). In addition, the backward whirl is heavily damped while the forward whirl is lightly damped. The first pair of rocking modes is similar to those found in disk/spindle systems with ball bearings and is lightly damped. The second pair of rocking modes occurs at low frequency. One of these modes is lightly damped and has natural frequency very close to half of the rotational speed. For the general case of a flexible shaft and coupled translation/rocking motion, eight coupled modes were obtained. Three of them occur at the half-speed frequency. Compared with systems with rigid shaft, the other five modes have significantly lower natural frequencies because of the shaft flexibility.
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