You mentioned verifying the results. I'm not sure if you were talking about by calculation or by test. I assume by test.
One way to confirm the results would be using a strobe if the vibrations are big enough to see. If you can freeze the shaft at that frequency then you can confirm the frequency and the shape.
Direct measurement of the frequency with an accelerometer and data collector would be nice as long as the accel is not so heavy that it changes the system. Also you could move the accel up and down to try to map the operating deflection shape.
I tried the calc again with revised numbers and still different thatn your results...I may have made an error.
Ishaft:=Pi/64*(Douter^4-Dinner^4);
IshaftVALUE:=subs({Douter=16*mm,Dinner=14*mm,Pi=pi},Ishaft);
IshaftVALUE := .133e4*mm^4
mu:=Pi*(Douter^2-Dinner^2)/4*rho;
muVALUE:=evalf(subs({Douter=16*mm,Dinner=14*mm,rho=1663*kg/m^3,Pi=pi},mu)*(m/(1000*mm))^2);
muVALUE := .780e-1*kg/m
ConversionVALUE:=kg/(m*second^2*Pascal);
EVALUE:=30000E6*Pascal;
LVALUE:=720*mm;
f1 := 1/(2*pi)*a1 * sqrt(E1*Ishaft1/(mu1*L1^4)*conversion);
f1:=subs({E1=EVALUE,Ishaft1=IshaftVALUE,conversion=ConversionVALUE,mu1=muVALUE,L1=LVALUE,a1=3.52},f1);
f1 = 24.3 hz
f2:=f1*22/3.52;
f2 = 152. hz
f3:=f1*121/3.52;
f2 = 836. hz
Anyone else have comments on the calcs or ways to confirm?
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