Module 8 : Transverse Vibrations of Multi-DOF Rotors

Lecture 4 : Transfer Matrix Methods with Gyroscopic effects and Dunkerley's Formula

The system natural frequency from the Dunkerley 's formula is given as

Using the TMM the value of the fundamental natural frequency was ωnf1 = 266.67 rad/sec. Hence, the Dunkerley 's formula estimates reasonably good estimate of the fundamental natural frequency, and it gives the lower bound.

Answer .

Example 8.11 Find fundamental transverse natural frequency of the rotor system shown in Figure 8.45. B1 and B2 are bearings, which provide simply supported end condition and D1 , D2 , D3 and D4 are rigid discs. The shaft is made of the steel with the Young's modulus E = 2.1 (10)11 N/m2 and uniform diameter d = 20 mm. Various shaft lengths are as follows: B1D1 = 150 mm, D1D2 = 50 mm, D2D3 = 50 mm, D3D4 = 50 mm and D4B2 = 150 mm. The mass of discs are: m1 = 4 kg, m2 = 5 kg, m3 = 6 kg and m4 = 7 kg. Consider the shaft as massless. Consider the discs as point masses.

Figure 8.45 A multi-disc rotor system

Solution : The influence coefficient for a simply support shaft with a disc is given as

(a)

where l is the span of the shaft, and a and b are the disc position from the left and right bearings. The natural frequency of a single-DOF rotor system can be obtained as

(b)

We have d = 0.02 m, l = 0.45 m, EI = 1649.34 N-m2 . Hence, EIl 3 =450.89 N-m5 . Table 8.6 summarises the calculation of the fundamental natural frequency.

Table 8.6 Calculation procedure of the fundamental natural frequency using the Dunkerley 's formula

Answer .

Exercise 8.12 Find transverse natural frequencies and mode shapes of the rotor system shown in Figure 8.46. B is a fixed bearing, which provide fixed support end condition; and D1 , D2 , D3 and D4 are rigid discs. The shaft is made of the steel with the modulus of rigidity E = 2.1 (10)11 N/m2 and the uniform diameter d = 20 mm. Various shaft lengths are as follows: D1D2 = 50 mm, D2D3 = 50 mm, D3D4 = 50 mm and D4B2 = 150 mm. The mass of discs are: m1 = 4 kg, m2 = 5 kg, m3 = 6 kg and m4 = 7 kg. Consider the shaft as massless. Consider the disc as point masses, i.e., neglect the diametral and polar mass moment of inertia of all discs.

Figure 8.46 A multi-disc overhung rotor

Solution : The influence coefficient for a cantilever shaft with a disc at free end is given as

(a)

where L is the span of the shaft. The natural frequency of a single-DOF rotor system can be obtained as

(b)