Negative Inductance and measure of Magnetic force.

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The backing magnet allows the inductive kickback to drive the piston back and trigger the spring switch. This motor is oscillating in Adams resonance at unity. A recycling diode would loop the reverse current. The reverse kickback is acting as an opposition switch. The throw is merely a few millimeters, but half the power is generated for free.

https://www.youtube.com/watch?v=9YqB3Genz3I

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Here's an earlier attraction oscillator in "Adam's Resonance" recovering BEMF:


The "Inductive Kickback" current reversal acts as a phantom sister "H" bridge switch!

https://www.youtube.com/watch?v=5SOHIUFgfxg

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The magnet piston can't travel past the center of the pulse coil core to work. This is an example of power from the delayed Lenz effect. I call it "Lenz Propulsion". The magnet stack gets a strong kick down free of charge; sufficient to trigger the spring switch and power the attraction stroke! The Flyback is generated from within the coil. The power stroke is delivered from the source outside the coil.

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One SPDT switch flyback reverse; The throw equals the length of the two magnet stacks and the connecting stator. This oscillator's power is awesome and over unity depending on the magnet strength and coil windings. The "Flyback" equals the strength of the attraction power stroke perhaps with the addition of a few backing magnets in attraction to the monopole. This may not be necessary.

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                                                                       Large disk magnets.

Here's a scaled up version of the Adams resonator: This so fiendishly simple no one's ever thought of it before. Half the operating power from "Inductive Kickback"! Think of the great amount of D.C. BEMF it would generate just chattering away with no heat loss.


The beauty of this "Flyback Monopole Oscillator" is that the COP is proportional to the weight in copper of the coil and the strength of the oscillating magnets.



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