ROTORDYNAMICS

'Rotordynamics' is a specialized branch of applied mechanics concerned with the behavior and diagnosis of rotating structures. It is commonly used to analyze the behavior of structures ranging from jet engines and steam turbines to auto engines and computer disk storage. At its most basic level rotordynamics is concerned with one or more mechanical structures (rotors) supported by bearings and influenced by internal phenomena that rotate around a single axis. The supporting structure is called a stator. As the speed of rotation increases the amplitude of vibration often passes through maxima that are called critical speeds. If the amplitude of vibration at these critical speeds is excessive catastrophic failure[1] occurs. In addition to this, turbomachinery often develop instabilities which are related to the internal makeup of turbomachinery, and which must be corrected. This is the chief concern of engineers who design large rotors.

Contents
Basic Principles
Jeffcott Rotor
History
References

Basic Principles


The equation of motion, in generalized matrix form, for an axially symmetric rotor rotating at a constant spin speed Ω is
:
egin{matrix}
Mddot{q}(t)+(C+G)dot{q}(t)+(K+H){q}(t)&=&f(t)\
end{matrix}

where:
''M'' is the symmetric mass matrix
''C'' is the symmetric damping matrix
''G'' is the skew-symmetric gyroscopic matrix
''K'' is the symmetric stiffness matrix
''H'' is the skew-symmetric circulatory matrix
in which ''q'' is the generalized coordinates of the rotor in inertial coordinates and ''f'' is a forcing function.
Both the gyroscopic matrix ''G'' and the circulatory matrix ''H'' are proportional to spin speed Ω.
The general solution to the above equation involves complex eigenvectors which are spin speed dependent.
Engineering specialists in this field rely on the Campbell Diagram to explore these solutions.

Jeffcott Rotor


The Jeffcott rotor (also known as the DeLaval rotor in Europe) is a simplified lumped parameter model used to solve these equations. Jeffcott's rotor was a mathematical tool that did not reflect actual rotor mechanics.

History


The history of rotordynamics is replete with the interplay of theory and practice. W. J. M. Rankine first performed an analysis of a spinning shaft in 1869, but his model was not adequate and he predicted that supercritical speeds could not be attained. In 1895 Dunkerley published an experimental paper describing supercritical speeds. Carl Gustaf De Laval, a Swedish engineer, ran a steam turbine to supercritical speeds in 1889, and Kerr published a paper showing experimental evidence of a second critical speed in 1916.
Henry Jeffcott was commissioned by the Royal Society of London to resolve the conflict between theory and practice. He published a paper now considered classic in the ''Philosophical Magazine'' in 1919 in which he confirmed the existence of stable supercritical speeds. August Föppl published much the same conclusions in 1895, but history largely ignored his work.
Between the work of Jeffcott and the start of World War II there was much work in the area of instabilities and modeling techniques culminating in the work of Prohl and Myklestad which led to the Transfer Matrix Method (TMM) for analyzing rotors. The most prevalent method used today for rotordynamics analysis is the Finite Element Method. One such program is DyRoBeS by Eigen Technologies [2].
Modern computer models have been commented on in a quote attributed to Dara Childs, "the quality of predictions from a computer code has more to do with the soundness of the basic model and the physical insight of the [analyst]. ... Superior algorithms or computer codes will not cure bad models or a lack of engineering judgment."
Prof. F. Nelson has written extensively on the history of rotordynamics and most of this section is based on his work.

References



Introduction to Dynamics of Rotor-Bearing Systems, Chen, J. G. , Gunter, E. J., , , , 2005, ISBN 1-4120-5190-8 uses DyRoBeS

Turbomachinery Rotordynamics Phenomena, Modeling, & Analysis, Childs, D., , , Wiley, 1993, ISBN 0-471-53840-X

Dynamics of Rotating Systems, Genta, G., , , Springer, 2005, ISBN 978-0-387-20936-4

The Lateral Vibration Loaded Shafts in the Neighborhood of a Whirling Speed. - The Effect of Want of Balance, Jeffcott, H. H., , , Philosophical Magazine, 1919

Dynamics of Rotors and Foundations, Krämer, E., , , Springer-Verlag, 1993, ISBN 0-387-55725-3

Rotordynamics Prediction in Engineering, Second Edition, Lalanne, M.,Ferraris, G., , , Wiley, 1998, ISBN 978-0-471-97288-4

Rotordynamics, Muszyńska, Agnieszka, , , CRC Press, 2005, ISBN 978-0-8247-2399-6

A Brief History of Early Rotor Dynamics, Nelson, F., , , Sound and Vibration, June, 2003

Rotordynamics without Equations, Nelson, F., , , International Journal of COMADEM, July 2007

Linear and Nonlinear Rotordynamics, Yamamoto, T.,Ishida, Y., , , Wiley, 2001, ISBN 978-0-471-18175-0

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