Magnetic Constant Motion Machine

ROTATION SPEED APPROX. 60 RPM.

B=KILOGAUSSE, H=OERSTEDS, T=TIME, Z=BEST CHARGING VALUE, Y=SURROUNDING FIELD VALUE

T1=.03 SEC ZB PULSE. HT1 =X

T2=.25 SEC. AFTER T1. HT2=X/<2 div="">

T3=.5 SEC. AFTER T1. HT3=0

ZH>YH * -1

ROUND BAR 4" X 1/2" DIAM. OR RECTANGULAR BAR 4"X 1/2" X 1/2".

SIZE REQUIREMENTS ARE FOR MANAGEABILITY AND ESTIMATED FIELD EFFECT CONSIDERATION.

The power force that the machine is intended to capture is sub-atomic movement. The spinning core material is a soft magnetic material to be determined.

This idea would only work if the force that turns the device (the field) is less that the coercive force to change the polarity of soft magnetic core. It would not be desirable to have the switcher or soft magnetic core change the magnetic force of the field, since its force is lower than that of the switcher then if would seem to be a magnetic material that may not be "charged" to its highest potienal. The gain being the distance the soft magnetic core traveled in the circumference and its increase in speed while in the magnetic field. This gain if any would have to overcome the magnetic grip that occurs when the poles are changed.
Image of apparatus using machined Magnetic Iron. No rotation with this material.
 

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