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Overunity Machines Forum



Oscillating sine wave LC tank magnet motor.

Started by synchro1, August 31, 2014, 09:26:50 AM

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0 Members and 5 Guests are viewing this topic.

MarkE

Quote from: synchro1 on September 08, 2014, 09:47:53 AM
Here's a definitive JLN video. JLN has completely mastered control of the "Lenz Delay Acceleration effect" by sliding the output coil along his "Barkhausen Core":


http://jnaudin.free.fr/dlenz/DLE21en.htm


Comments :
We notice on the curve below, that the braking effect (common Lenz effect) and the accelerating effect (reverse Lenz effect) of the rotating magnetic rotor (blue curve) is DIRECTLY LINKED to the phase shifting curve of the magnetic fluctuation (red curve). The acceleration of the rotor is maximal when the phase angle switches from postive to negative (the green rectangle area at a distance of 30mm). The loaded secondary coil is set at the phase shifting point and acts as a wave reflector, it returns the magnetic wave in opposition phase to the magnetic rotor in rotation, producing its acceleration.
The experiment that you are looking at demonstrates different amounts of power shunting.  If you allow your car engine to idle with the car in gear it will move forward with a small amount of pressure on the brakes, and more quickly with less pressure on the brakes.  The engine efficiency is unchanged by what you do with the brakes.  If you were to put a motor and a cam on the throttle, the car would then accelerate in an undulating pattern.  If you time application of the brakes you could arrange that the brakes are pressed hardest when the throttle is open and the least when the throttle is closed, or alternately the most when the throttle is closed and the least when the throttle is open.  The average speed will be differnt between the two cases, but engine efficiency is still unaltered.

And so it is here.  One can reduce the losses and due to the magnetic viscosity, one can also time the phase relationship between the braking and acceleration forces to coincide at maximum or at opposition.  What one cannot do is convert the braking forces into self-accelerating forces.

synchro1

@MarkE,

Quote from you:

"What one cannot do is convert the braking forces into self-accelerating forces".

So what?

MarkE

Quote from: synchro1 on September 08, 2014, 04:43:07 PM
@MarkE,

Quote from you:

"What one cannot do is convert the braking forces into self-accelerating forces".

So what?
So, what is that as much fun as magnetic viscosity may be, it is a loss mechanism.  More of the effect does not improve efficiency, it hurts efficiency.

synchro1

@MarkE,


Help solve this one: Suppose JLN's pulse power input is many times greater then sine wave drive. Accepting that we can accelerate the spinner to 25k both ways; Would the "Magnet Wave Reflector Coil" behave any differently with one power source over the other?   

MarkE

Quote from: synchro1 on September 08, 2014, 07:35:50 PM
@MarkE,


Help solve this one: Suppose JLN's pulse power input is many times greater then sine wave drive. Accepting that we can accelerate the spinner to 25k both ways; Would the "Magnet Wave Reflector Coil" behave any differently with one power source over the other?   
If speaking only in terms of the driving waveform, a sine wave source with the same peak amplitude as a square wave source will be free of harmonics that mostly just waste power.