Rotor Bearing System Analysis Using the Transfer Matrix Method with Thickness Assumption of Disk and Bearing
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Rotor Bearing System Analysis Using the Transfer Matrix Method with Thickness Assumption of Disk and Bearing

Authors: Omid Ghasemalizadeh, Mohammad Reza Mirzaee, Hossein Sadeghi, Mohammad Taghi Ahmadian

Abstract:

There are lots of different ways to find the natural frequencies of a rotating system. One of the most effective methods which is used because of its precision and correctness is the application of the transfer matrix. By use of this method the entire continuous system is subdivided and the corresponding differential equation can be stated in matrix form. So to analyze shaft that is this paper issue the rotor is divided as several elements along the shaft which each one has its own mass and moment of inertia, which this work would create possibility of defining the named matrix. By Choosing more elements number, the size of matrix would become larger and as a result more accurate answers would be earned. In this paper the dynamics of a rotor-bearing system is analyzed, considering the gyroscopic effect. To increase the accuracy of modeling the thickness of the disk and bearings is also taken into account which would cause more complicated matrix to be solved. Entering these parameters to our modeling would change the results completely that these differences are shown in the results. As said upper, to define transfer matrix to reach the natural frequencies of probed system, introducing some elements would be one of the requirements. For the boundary condition of these elements, bearings at the end of the shaft are modeled as equivalent spring and dampers for the discretized system. Also, continuous model is used for the shaft in the system. By above considerations and using transfer matrix, exact results are taken from the calculations. Results Show that, by increasing thickness of the bearing the amplitude of vibration would decrease, but obviously the stiffness of the shaft and the natural frequencies of the system would accompany growth. Consequently it is easily understood that ignoring the influences of bearing and disk thicknesses would results not real answers.

Keywords: Rotor System, Disk and Bearing Thickness, Transfer Matrix, Amplitude.

Digital Object Identifier (DOI): doi.org/10.5281/zenodo.1332778

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References:


[1] Rao, S.S., 1983, Rotor Dynamics, John Wiley & Sons, Newyork
[2] Pestel, E. C., and Leckie, F. A., 1963, Matrix Methods in Elastomechanics, McGrawHill, New york.
[3] Prohl, M. A., 1945, "A General Method for Calculating Critical Speeds of Flexible Rotors", ASME J. Appl. Mech., Vol. 67, p. 142.
[4] Lund, J. W., and Orcut, F.K., 1967, Calculations and Experiments on the Unbalance Response of a Flexible Rotor, ASME Journal of Engineering for Industry, Vol. 89 (4), pp.785-596.
[5] Bansal, P. N., and Kirk, R. G., 1975, "Stability and Damped Critical Speeds of a Flexible Rotor in Fluid Film Bearings," ASME J. Ind., Series B, 97(4), pp. 1325-1332.
[6] Tan, C.A., Kang. B., 1999, Free vibration of axially loaded, rotating Timoshenko shaft systems by the wave-train closure principle, International Journal of Solids and Structures, Vol 36, pp. 4031-4049.
[7] Meriam, J.L, Kraige L.G, 1998, Dynamics, John Wiley & Sons, New york.
[8] Beer, F.P, Johnston, J.R., 1992, Mechanics of materials, Mc Graw Hill, Singapore.
[9] Timoshenco, S. P., Goodier, J.N., 1970, Theory of Elasticity, 3rd Ed., McGraw-Hill.