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Effects of Shaft Flexibility and Gyroscopic Coupling on Instability Threshold Speeds of Rotor-Bearing Systems

机译:轴柔性和陀螺耦合对转子系统不稳定性阈值速度的影响

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The driving speeds at which self-excited motions occur in rotor-bearing systems are commonly referred to as "instability threshold". These speeds and the magnitude of rotor (journal) trajectories are two important variables characterising the limits and states of a rotating machinery. The hydrodynamic lubrication in journal-bearing provides damping and reduces friction on rotor systems; therefore the journal amplitude should not exceed the bearing radial clearance. Linear bearing models are not able to accurately predict the journal trajectories for rotor-bearing system operating in conditions where the system does not have period one solutions, or when the journal motion is larger than 20-30% of the bearing radial clearance. Therefore the nonlinear bearing impedance descriptions method was used to model the hydrodynamic reaction forces. Two cases were analysed: 1) a rigid non-symmetric rotor and 2) a flexible non-symmetric rotor. The two models consist of a rotor supported by two identical finite-length hydrodynamic journal bearings of length to diameter ratio L/D=1, with same lubricant properties. The flexible non-symmetric rotor was modelled by the finite element method (FEM). Simulation results show that the instability threshold of the rigid non-symmetric rotor-bearing system (case1) depends on the low stability characteristics of the less loaded bearing. But when the shaft flexibility and the gyroscopic coupling effect are taken into account; the instability threshold increases for the flexible non-symmetric rotor-bearing system (case2). The gyroscopic coupling effect does not only increase the instability threshold, but the journal trajectories magnitude has also significantly increased. This is normally not a preferable condition since high vibrations will induce heat and stress in babbited bearing.
机译:转子承载系统中发生自激动运动的驱动速度通常被称为“不稳定性阈值”。这些速度和转子(日记)轨迹的大小是两个重要变量,其特征在于旋转机械的限制和状态。轴颈中的流体动力润滑提供阻尼并减少转子系统的摩擦;因此,轴颈幅度不应超过轴承径向间隙。线性轴承模型无法准确地预测转子轴承系统的轨迹,在系统没有使用期间一种解决方案的条件下操作,或者轴颈运动大于轴承径向间隙的20-30%。因此,非线性轴承阻抗描述方法用于模拟流体动力反应力。分析了两种情况:1)刚性非对称转子和2)柔性非对称转子。这两种型号由两个相同的有限长度流体动力轴承支撑的转子组成,长度为直径比L / D = 1,具有相同的润滑剂性能。柔性非对称转子由有限元方法(FEM)建模。仿真结果表明,刚性非对称转子轴承系统(壳体1)的不稳定性阈值取决于负载轴承较少的低稳定性特性。但是当考虑轴灵活性和陀螺仪耦合效果时;柔性非对称转子轴承系统(壳体2)的不稳定性阈值增加。陀螺仪耦合效果不仅增加了不稳定性阈值,而且轴颈轨迹幅度也显着增加。这通常不是优选的条件,因为高振动将引起粘性轴承中的热量和应力。

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