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Mechanical Magnetic Torque Amplifier

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  • The separated wave form below shows where we would position the monopole magnet on the ferrite oscillator driver to benefit from "Lenz Propulsion". The SPDT switch would be positioned to trigger exactly there. The magnet on the other end would be in the center of the coil awaiting the pulse; Centered so it would attract on one side and repel on the other.



    Last edited by Allen Burgess; 04-22-2019, 01:07 AM.

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    • Microwave door switch wedged in PVC "T" with a chopstick. You can see the magnet piston depressing the switch button on the bottom.



      Last edited by Allen Burgess; 04-23-2019, 07:06 AM.

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      • Switch button from the top:

        Last edited by Allen Burgess; 04-23-2019, 07:07 AM.

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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
          Last edited by Allen Burgess; 04-22-2019, 11:52 PM.

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          • BEMF recovery

            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
            Last edited by Allen Burgess; 04-23-2019, 08:26 AM.

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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.

              Last edited by Allen Burgess; 04-23-2019, 09:58 PM.

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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.

                Last edited by Allen Burgess; 04-24-2019, 04:56 PM.

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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.

                  Last edited by Allen Burgess; 04-24-2019, 05:40 PM.

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                  • Here is a Gotoluc version; Two coils of different wire gauge in series. The secondary is connected in series with the primary through a diode and the capacitor. This prolongs the time interval like Woppyjump does in his BEMF rotor build. A reed switch could handle this two pulse oscillator:

                    Last edited by Allen Burgess; 04-25-2019, 05:29 PM.

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                    • Coil Jouncer.

                      I built the oversized flyback oscillator with radial ceramic micro wave oven magnets and discovered that it's much easier and more efficient to oscillate the coil between the large disc magnets.

                      This multiplies the BEMF output tremendously. Do the math: An Adams resonator between two powerful disc magnets of one pound of copper and X amount of magnet strength with one watt of input would double it's COP with two pounds of copper on the coil.
                      Last edited by Allen Burgess; 04-26-2019, 12:00 AM.

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                      • Comment


                        • piezo transducer mounted on oscillator.

                          The Piezo transducers can buffer the switches:

                          Last edited by Allen Burgess; 05-08-2019, 04:24 PM.

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                          • Gotoluc's magnet advantage

                            Gotoluc demonstrates the power advantage additional magnets add to his traveling coil:


                            https://www.youtube.com/watch?v=OxuotFUWVGQ

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                            • Adams

                              Adding magnet strength to the MMM (Mostly Magnet Motor) increases inductive kickback along with coil torque. Luc adds a latching relay to his SPDT switches. Inductive kickback increases with frequency of power interruption. The "Echo Canyon" of Adams resonance, not the mechanical throw, is where the COP advantage is greatest with this kind of super build.

                              Oscillating in Adam's resonance, the "Inductive Kickback" delivers half of the motor power! Vibration transducers provide a superior output in the millimeter throw range.
                              Last edited by Allen Burgess; 05-11-2019, 12:53 PM.

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                              • Current reversing monopole

                                What would this current reversing monopole oscillator be called? Too bad he can't get the magnet rod to work his switch.

                                https://www.youtube.com/watch?v=ys2-wTU5w4E
                                Last edited by Allen Burgess; 05-13-2019, 11:04 AM.

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