Guineafowl
- 963
- 422
The mill motor in delta.
I need to see the data points to know if it shows the zoomed in sampling rate, or the real rise time.Guineafowl said:2. Pulses (occurring at 8 kHz) have a rise time of 6.56 us:
I can see the motor drive sinewave in that plot.Guineafowl said:3. + filter, output overview:
It looks like you zoomed too far into a waveform, until we see the data acquisition rate. That does not show the slope dv/dt, of the motor drive waveform, which should have been reduced by the LPF.Guineafowl said:4. Pulses had an irregular appearance:
8 kHzBaluncore said:What is the frequency of the PWM output.
Configured as per post #35, the caps are in delta and had to be replaced with 2.2 nF, as the 0.47 uF ones were tripping the VFD. Do you mean the LPF in the VFD? I haven’t been able to find that out.Baluncore said:What is the cutoff frequency of the low-pass filter.Baluncore said:What is the Y filter centre connected to, or is it floating?
The VFD was expecting to drive an inductive motor. You raised the frequency of the LPF by 470 / 2.2 = 200 times. That explains why the dv/dt is higher than I expected. There is little point using that filter in that situation. You would need to increase the inductance to compensate.Guineafowl said:Configured as per post #35, the caps are in delta and had to be replaced with 2.2 nF, as the 0.47 uF ones were tripping the VFD.
No. Impedance is a vector sum of resistance and reactance, ( R + j X ).Guineafowl said:Would this represent a motor impedance per phase of 240/3.1 =77.4 Ω ?
Isn’t the full-load rms current of 3.12 A a consequence of the effective, or apparent, impedance under these conditions? As far as I can find out from motor control technical articles, this is the figure used to derive the 3% or 5% reactor impedance target.Baluncore said:No. Impedance is a vector sum of resistance and reactance, ( R + j X ).
An induction motor has a small reactive current in quadrature with the voltage, that current magnetises the field inductance.
There is also an inphase current that provides the real power to the motor. That is shaft power plus windage, friction and resistive I2R loss. The real current is dependent on mechanical load, and is significantly more than the load independent magnetising current.
You need to look at the power factor under no load and full load, to separate those numbers.