From my perspective reading Krauss, it applies to large squirrel cage motors since they have high L/R ratio, especially in the rotor circuit. It also applies during rapid changes (in addition to DOL start, he also shows example of slight ringing on the large motor during rapid load change and during external fault which is quickly cleared).
It would not apply to smaller motors since they have lower L/R (for example see the 50hp startup curve in attachment above - no overshoot). It would not apply to vfd start since the speed is slowly ramped. It would not apply to slip ring motor if: 1 - speed is increased slowly, or 2 - motor is small. If there is large slip ring motor started DOL, I suppose it's a possibility although I think rotor resistance is higher for slip ring motors than squirrel cage motors.
I was able to do a simulation which matched the results posted. I will posts some results from there to show a slightly different view: speed vs time and torque vs time. The thing that confuses me a little bit is the time constants. For this 2250hp motor with R2' ~ 0.02, XL2' ~ 0.2, Xm ~ 13, which has L/R on the high (long) end of the spectrum, it still seems to have a fairly small/short time constant. Using the the rotor leakage inductance:
Rotor L/R = L'/R' = Xl' / R' /(2*PI*60) = (0.2/0.02) / 377 ~ 0.025 sec.
That seems relatively short in comparison with the transient and the oscillation a..........
Now if for some reason you included Xm in the ratio the time constant would be a lot longer (but it's not obvious that should be included)
Rotor L/R = L'/R' = Xl' / R' /(2*PI*60) = (13/0.02) / 377 ~ 1.5 sec.
At this point it doesn't quite make sense to me - I can't reconcile the time constant with the transient. Maybe my question will be clearer to readers when I post the plots vs time (maybe tonight).
=====================================
Eng-tips forums: The best place on the web for engineering discussions.