Has anyone yet considered that some of the coils are physically shorted at certain parts of the cycle?
And how this affects the dynamics of inductance, flux, and saturation as energies are circulated around the transformer?
Mechanical relay contacts are not instant make/break. Especially when de-energizing, there is a delay of many milliseconds before the relay contact is physically broken. Based on the switching diagrams I've seen, it seems likely that there can be periods of coil-shorting at certain phases of a cycle.
Coil-shorting results in parametric variation of inductance (ie: Mag-Amp). Parametric variation of L and/or C is a fundamental note in much of Eric Dollard's writings.
So what happens when we try to model and simulate a rotary transformer that is also a mag-amp? 
(just a quick thought I've been pondering as I work on my own experiments)
I see this all in a different light as to what is being done. The full circuit has not been given, AFAIK, but was given a small diagram which if looked at well resembles a boost circuit. If so, then part of the voltage is sent to the capacitors and the other to the next coil, I use this myself for other devices, yes parametric if the capacitor is across two adjacent coils. Charge one and discharge two, the result is the change in inductance of one coil into two coils which actually gives you X4 the inductance when there is a core. By doing this using one mosfet for two coils, connected between two coils, there will be a natural progression around the stator, fisical polarity changing in my view is not needed, this is similar to Figura. Regards Mike 
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Topic: Pierre's OU claim (Read 32228 times)
