Module 8 : Transverse Vibrations of Multi-DOF Rotors

Lecture 1 : Influence Coefficient Method

Equation (e) has the following form

(f)

Hence, for a = 0.075 m, L = 0.125 m, N-m2 , we have

(g)

The deflection at station 2 can be obtained as

(h)

On substituting equations (a) and (b) into equation (h), we get

which finally takes the form

(i)

Equation (i) has the following form

(j)

Hence, for a = 0.075 m, L = 0.125 m, EI = 103.1 N-m2 , we have

(k)

Method of the singularity function : Now the influence coefficients are obtain by the method of singularity function for illustration. The singularity function (< >) is defined as

 

(l)

The bending moment at any cross-section along the shaft span can be written as

(m)

which implies that for 0 ≤ z a contribution from the Fy2 would not be there since ( z – 0.075) would be a negative quantity so it becomes zero. However, for az L contributions from both Fy1 and Fy2 would be there. On integrating twice equation (m), we get following expressions

(n)

and

(o)

where the integration constants c1 and c2 are obtained by boundary conditions of the probelm, and are give as

 

 

 


(p)

 

 

 

 

(q)

Finally equation (o) becomes

(r)