Mechanical Magnetic Torque Amplifier

[Allen Burgess]

Here we see the two coils and magnets: The primary against the wall pulses the ring magnets on the levitator axle, and the second larger coil collects the BEMF from the first between the powerful horse shoe uprights. The scale up of magnet force and coil mass on the center axle is designed to magnify the magnetic field of the center coil to compensate for the lesser amount of BEMF power while delivering a back stroke of equal strength:

This linear oscillator can use a diode and capacitor like Gotoluc, along with one side of the SPDT spring pressure switch instead of Luc's Reed switch. Either way there's a delay between the power pulse in the primary coil and the power pulse in the secondary;

[Allen Burgess]

Woopyjump's BEMF spinner; Look at and compare the relative size of the coils and cores: These are the same proportions the two coils would need to be on the linear oscillator. The degree of offset from 90 degrees is the delay that would equal the throw for the oscillator.

The linear oscillator would allow us to keep the coils the same size, if we increase the magnet strength of the horse shoe. We can reinforce the field by adding magnets to the outside of the stators while keeping a tight gap for the coil:

The oscillator, although asymmetrical, corrects Gotoluc's imbalance issue.

[Allen Burgess]

The larger coil at 2 O'Clock is the primary. The one on the left is powered by the backspike. That one would ride on the axle. The switch wires between the negative and the bottom of the coil:

[Allen Burgess]

The circuit interrupts at the base of the primary coil, just like luc's circuit, and the 12 volt zener diode allows the high voltage backspike to pass to the high voltage secondary while protecting it from the 9 volt battery. There's no capacitor. Luc has a tiny pico farad capacitor in parallel with the secondary. This is basically the same circuit with a transistor. The spring pressure switch can trigger the transistor in place of Lynx's commutator.

[Allen Burgess]

1st Mendocino Oscillator run

https://youtu.be/2VhQq_utlQg

Looks pretty simple until you consider that there's a live output wire leading away from the pulse coil.

[Allen Burgess]

Lynx Joule Motor.

The chief advantage of the "Lynx Joule Motor" circuit over gotoluc's is the recycling of bemf from the secondary to the source battery though a bridge rectifier. Luc's circuit fails to pass the gain on. We get a two for one advantage with the secondary, and a third with Lynx's looped charge.

[Allen Burgess]

Reciprocating twin.

Two reciprocating solenoid coils of different sizes and strength magnet pistons connected to a yoke would deliver the equal force stroke with the lynx joule motor BEMF return circuit just tied together, without the levitator. An elliptical cam lobe could correct for unequal throw distances of equal force. Doubling the copper mass and magnet strength would naturally multiply the flywheel torque.

[Allen Burgess]

axle coil and horse shoe.

[Allen Burgess]

motor alternator;

[Allen Burgess]

[Allen Burgess]

Secondary neutralization pulse

This configuration above uses an attraction neutralization force on each end, and adds core advantage to the center coil.

[Allen Burgess]

Coil core suspended from magnet stator.

[Allen Burgess]

Back spike power stroke.

The Axle coil needs to generate sufficient magnetic force from the primary flyback to free the core attraction to the magnet stator. The attraction to the stator can be controlled by adding or subtracting ceramic blocks along with the inclusion of a spacer. This will free the axle to attract to the opposing backing magnets with sufficient force to depress the spring pressure switch. This attraction force can be controlled by adding or subtracting magnets along with a spacer too. Balanced opposing attractions along with two attraction neutralization pulses.

The primary is charged by a 3055 transistor from a 9 volt battery, connected through the switch to the transistor base through a resistor. The high voltage flyback from this power assisted pulse, is passed to the secondary axle coil through a zener diode.

The BEMF that charges the 9 volt run battery from the secondary through a FWBR would generate as a lower voltage inductive type with input polarity Current.

This would be a genuine unity motor generator, the overall output of which would multiply from scale up.

[Allen Burgess]

Balance of opposing attraction forces.

Asymmetrical geometry delivering symmetrical force.

[Allen Burgess]

Same throw 20% of the power

This is the last and most definitive video in Luc's recycled flyback series.

https://www.youtube.com/watch?v=7QUYkilgkzU