An analysis of the self-excited oscillations, known as “oil whip,” of a rotor supported in fluid film bearings is presented. The source of the instability is the hydrodynamic forces of the bearing fluid film. The equations of motion are nonlinear, and they are studied to determine the limit cycles of the system, also called the whirl orbits. The nonlinear equations are solved by the method of averaging whereby the whirl orbits are obtained directly. The results are dimensionless and are given in graphical form. They show under which conditions whirl orbits can exist, and the position and the size of the orbits are also given. It is found that the orbits are only encountered in a relatively narrow speed interval around the speed at which the static equilibrium becomes unstable.
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November 1967
This article was originally published in
Journal of Engineering for Industry
Research Papers
Oil Whip Whirl Orbits of a Rotor in Sleeve Bearings
J. W. Lund,
J. W. Lund
Vibrations and Acoustics, Mechanical Technology Inc., Latham, N. Y.
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E. Saibel
E. Saibel
Department of Mechanics, Rensselaer Polytechnic Institute, Troy, N. Y.
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J. W. Lund
Vibrations and Acoustics, Mechanical Technology Inc., Latham, N. Y.
E. Saibel
Department of Mechanics, Rensselaer Polytechnic Institute, Troy, N. Y.
J. Eng. Ind. Nov 1967, 89(4): 813-823
Published Online: November 1, 1967
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Received:
December 1, 1966
Online:
August 25, 2011
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Lund, J. W., and Saibel, E. (November 1, 1967). "Oil Whip Whirl Orbits of a Rotor in Sleeve Bearings." ASME. J. Eng. Ind. November 1967; 89(4): 813–823. https://doi.org/10.1115/1.3610159
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