Thanks to all for your feedback again.
BobM3 : Thanks for the reference to thread on rubber spring rate.Interesting.
I am little confused with the use of "dynamic stiffness" terminology being used in this scenario. I am aware of using (K-mw^2+iwC)as dynamic stiffness for a conventional academic SDOF model. Does this hold good in the context of coupling dynamic torsional stiffness as well? The manfr often gives this value and depedency on frequency factors and temperature influences as rightly said by Rob 768.
Or is this a two step approach? Meaning,we get the dynamic torsional stiffness assuming coupling as a individual system (which is normally calculated and provided by manfr). Then we use this dynamic stiffness in the drive train torsional analysis.
electricpete: That is exactly my doubt.
In linear dynamic systems, in the (K-mw^2+iwC), when w-->0, the stiffness what we arrive is the static stiffness.
Say from 10 - 50Hz at low frequencies where the system's coupling torsional mode normally lies (where the coupling manfr usually gives the dynamic torsional stiffness data), is it good to assume that the dynamic stiffness is K+iwC (Greg, is that your argument?).
My problem is from the measured torsional stiffness, say from static test or by bump test, can I estimate the dynamic torsional stiffness at my excitation frequency of interest?
Can I say we can approach this in two ways?
1)Measure static torsional stiffness (measuring torque/deflection) using rotor1-coupling-rotor-2 setup. Then estimate the dynamic torsional stiffness as (K+iwC) at excitation frequency w and use that for torsional analysis calculation
2)with Bump test, get the dynamic stiffness directly at the excitation frequency from the frequency response function and use the same for torsional calculations
Only thing in both cases is that I can't see the amplitude and frequency effect of torsional stiffness?
Your suggestions and opinions, please
Jeyaselvan