Torsional Vibration of Turbomachinery

Appendix A: Mathematical Model for a Geared System

This appendix shows by means of a simple example the way in which a multispeed geared system is transformed into an equivalent single-speed system.

The equivalent system must be constructed to have identical torsional natural frequencies to the geared system. The geared system mode shapes and forced response values are derived from the results from the equivalent system using the transforms that are developed in this appendix.

Figure A.1 shows a simple geared torsional model for illustration purposes with speed increase gears I 2 and I 3 between two rotors, I 1 and I 4.


Figure A.1: Mathematical model of geared system.

The rotor system I 3- I 4 rotates N times faster than the rotor system I 1- I 2, as a result of the gears. Hence the velocity ratio of I 1- I 2 is 1 and that of I 3- I 4 is N.

Angles ? 1 through ? 4 are the rotational displacements at each rotor or gear location. T 1 and T 4 are applied torques acting on rotors 1 and 4, respectively. T G 2 and T G 3 are gear mesh torques acting on gears I 2 and I 3, respectively. k 1 and k 2 are the shaft stiffnesses.

Figure A.2 shows the equivalent single speed model where J 1, J 2, and J 4

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