Second natural frequency can be simplified as
| (q) |
with
It should be noted that equation (q) is exactly the same as in previous example (i.e., for equivalent two mass rotor system) for which . For the present example problem, natural frequencies are expected to be reduced because of the increase in the polar mass moment of inertia of the system; moreover, there is an increase in DOFs of the system to three from two of Example 6.11.
Example 6.13 Obtain torsional natural frequencies and mode shapes of a branched system as shown in Figure 6.42. The polar mass moment of inertia of rotors are:.Gear ratios are:
. Shaft lengths are:, and diameters are
Take the modulus of rigidity of the shaft as
.
Figure 6.42 A branched rotor system
Solution: The branched system has the following numerical data
For branch AB, state vectors at stations are related as
with