Hello Ron,
Good to see that you are becoming engaged with the ZFM concept. Your experiments are definitely worthwhile in that they clarify the workings of the fields in the static mode. Perhaps you should consider that these fields becoming modified in the dynamic mode and that the magnitude of their respective influences become different also. I assume (I may be wrong) that for classical DC motors the strength of the induced electrical field within the coil diminishes as the RPM increases - so according to "Hoyle" the maximum RPM (no applied load) is reached when the applied force on the rotor from the induced field is equaled to the total of internal friction, windage (air resistance) and BEMF.
But with the ZFM (depending on input voltage, timing parameters, etc) once this point is reached the machine will normally run up to and at this balanced level for several minutes, shorter or longer, when there is a tangible acceleration. This acceleration can appear in steps increasing the RPM about 10 -20%. So apparently all the restraining forces are somehow reduced or the input is increased. Must be the smoke and mirrors...
One can suggest that the true magnetic lines of force now come into play. Another proposed explanation could be that certain resonant points are activated within the machine above a certain firing frequency. Still shooting in the dark with all this, but persistent and careful experimentation will slowly clarify these issues. The interaction of the different fields certainly makes this a very interesting machine.
It is worthwhile to note that while the machine is in this hyper mode, the position of the firing point (energizing the coils) can be moved over a 35-40 degree range with minimal impact on RPM and amperage draw. At slow RPM's this type of adjustment has a dramatic impact on speed and amp draw.
So the Green lines may yet rule - Happy Halloween!
Yaro
Good to see that you are becoming engaged with the ZFM concept. Your experiments are definitely worthwhile in that they clarify the workings of the fields in the static mode. Perhaps you should consider that these fields becoming modified in the dynamic mode and that the magnitude of their respective influences become different also. I assume (I may be wrong) that for classical DC motors the strength of the induced electrical field within the coil diminishes as the RPM increases - so according to "Hoyle" the maximum RPM (no applied load) is reached when the applied force on the rotor from the induced field is equaled to the total of internal friction, windage (air resistance) and BEMF.
But with the ZFM (depending on input voltage, timing parameters, etc) once this point is reached the machine will normally run up to and at this balanced level for several minutes, shorter or longer, when there is a tangible acceleration. This acceleration can appear in steps increasing the RPM about 10 -20%. So apparently all the restraining forces are somehow reduced or the input is increased. Must be the smoke and mirrors...
One can suggest that the true magnetic lines of force now come into play. Another proposed explanation could be that certain resonant points are activated within the machine above a certain firing frequency. Still shooting in the dark with all this, but persistent and careful experimentation will slowly clarify these issues. The interaction of the different fields certainly makes this a very interesting machine.
It is worthwhile to note that while the machine is in this hyper mode, the position of the firing point (energizing the coils) can be moved over a 35-40 degree range with minimal impact on RPM and amperage draw. At slow RPM's this type of adjustment has a dramatic impact on speed and amp draw.
So the Green lines may yet rule - Happy Halloween!
Yaro
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