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Oil whirl, oil whip and whirl/whip synchronization occurring in rotor systems with full-floating ring bearings

机译:带全浮动环形轴承的转子系统中发生油涡流,油鞭和涡流/鞭子同步

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摘要

High-speed rotors are often supported in floating ring bearings because of their good damping behavior. In contrast to conventional hydrodynamic bearings with a single oil film, full-floating ring bearings consist of two oil films: An inner and an outer oil film. As single oil-film bearings, full-floating ring bearings also show the typical fluid-film-induced instabilities (self-excited vibrations). Both inner and outer oil films can become unstable and exhibit oil whirl/whip instabilities. The paper at hand considers a Laval (Jeffcott) rotor, which is symmetrically supported in full-floating ring bearings, and investigates the occurring oil whirl/whip effects by means of run-up simulations. It is shown that the inner oil film, which usually becomes unstable first, gives rise to a limit-cycle oscillation with an exactly circular rotor orbit, if gravity and imbalance are neglected. Interesting is the instability generated by the outer oil film. The calculations demonstrate that instability in the outer oil film does not lead to a simple circular limit-cycle orbit. Whirl/whip-induced limit-cycle oscillations generated by the outer oil film are more complex and entail a coupled circumferential and radial motion, although the mechanical problem is radially symmetric, if gravity and imbalance are neglected. Thus, whirl/whip instability in the outer fluid film may be interpreted as symmetry breaking. Finally, a further kind of bifurcation/instability occurring in rotors supported in full-floating ring bearings-called Total Instability in this paper-is analyzed. It is shown that Total Instability is caused by synchronization of two limit cycles, namely synchronization of the inner and outer oil whirl/whip. Total Instability is of practical interest and observed in real technical rotor systems, and frequently leads to complete rotor damage.
机译:高速转子通常由于其良好的阻尼性能而被支撑在浮动环轴承中。与具有单个油膜的常规流体动力轴承相比,全浮动环轴承由两个油膜组成:一个内部油膜和一个外部油膜。作为单油膜轴承,全浮动环轴承也显示出典型的由液膜引起的不稳定性(自激振动)。内油膜和外油膜都可能变得不稳定,并表现出油涡动/鞭状不稳定性。这篇论文考虑了一个拉瓦尔(Jeffcott)转子,该转子对称地支撑在全浮动环形轴承中,并通过运行模拟研究了发生的油回旋/甩动效应。结果表明,如果忽略重力和不平衡,通常首先变得不稳定的内部油膜会在转子轨道正好为圆形的情况下引起极限循环振荡。有趣的是外油膜产生的不稳定性。计算表明,外油膜的不稳定性不会导致简单的圆形极限循环轨道。尽管忽略了重力和不平衡,虽然机械问题是径向对称的,但由外部油膜产生的由涡流/鞭子引起的极限循环振荡更为复杂,并伴随着周向和径向运动的耦合。因此,外部流体膜中的旋转/旋转不稳定性可以解释为对称破坏。最后,分析了在全浮动环形轴承中支撑的转子中发生的另一种分叉/不稳定性,在本文中称为“总不稳定性”。结果表明,总不稳定性是由两个极限循环的同步引起的,即内部和外部油涡流/鞭子的同步。完全不稳定性具有实际意义,并且在实际的转子技术系统中已观察到,并且经常导致转子完全损坏。

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