CMOS Oscillator

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                                                                                                                                     CMOS Complimentary MOSFETs.

A reverse biased Hi voltage P channel Mosfet in depleton mode and a depletion mode N channel on both power and ground sides of an electromagnet coil with the gates connected would both turn off at the ground side and simultaniously turn on at the power side to conduct the high voltage back spike to storage. The coil generates a magnetic field frrom the current interupted collapse. Input diode directed to same power wire. Approaching the electrode coneccted to the two gates with a ground wire would both interrupt the current to the charged coil at the ground and turn on the hi voltage mosfet connected to the storage capacitor. The magnetic field can power an oscillator carrying the negative ground wire that triggers the gates. A timer circuit can deliver this pulse also.

This circuit is a Little tricky because the first Mosfet is wired backwards. The field polarity is reversed in the coil when the input returns from source. This generates an AC signal and acts as an inverter. This is our basic logic circuit with information stored in the normally closed position with no power requirement. The combination of the collected current and the forcé from the magnetic field is an overunity event.

These two Mosfets have vastly different characteristics. It is simple to imagine a magnet piston AC motor that runs for free. Amperage frequency pounds of copper and magnet strength would determine wether you would run a luxury liner or a wrist watch. Position the ground wire between the gates electrode on the coil face and the magnet pendulum attached to the magnet pendulum or piston. A third mosfet on the input could gate trigger at TDC delay the incomming pulse and lengthen the throw. A Newman moter could run with the three CMOS and ground trigger commutator leveraging full use of the backspike magnet field..

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Shuttling an axial tube magnet between 2 coils each side with 3 Mosfet gates connected to an electrode and a ground contact in close adjacency. The Mosfet sensitivity would easily trigger from the proximity of the shuttle magnet.


The contact from the input on the opposite end would join the interruptor.

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Anyone can add up the 150% overunity! 2 of the 4 power pulses are double work. That is 1/2 for free! The primary input mosfets would both need timers. 4 diodes too. A Newman motor would run off the same circuit!

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Two Reed switches would handle the input more easily, one on the top to charge the opposite coil a another to shut it off. The interruptor is the Mosfet, but the coil should be off to not fight the ascent tail and lengthen the throw.

We don't need the opposite coil to turn back on right away. It needs to be on only one way.


The other approach would be to make the ground a latching Mosfet by including a Capacitor and resistor.

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2 latching Reed switches and 4 tiny trigger magnets can lengthen the power pulse. The simultaneous switching of the Mosfets is necessary to recover the full back spike. Keeping the current on to the attraction coil can be most easily handled with a couple of these kind of switches which have wider Latitude.

We can't use this top side switch to interrupt the current to collect backspike. This is the single most common reason why builders fail at successful self runners. Think about the problem!