Resonance collection

The following is a Systematic investigation into circuit ideas to establish resonance collection from the RV’s one phase power for OU. To date nearly all circuits from PHIL and RAIVO have been tested and work. A select group experienced in testing resonance extraction lay emphasis on the concept that over unity can result from the voltage node or ‘peaks’ from a resonance source. Certainly by an understanding and use of magnetism and capacitors one can contemplate the many ways in which an over unity result is possible. Currently to conserve the resonance processes and enable proper amplification and tame the phenomena for extraction a research community of non corporate vision have been researching and developing Hectors RV or rotor-conversion effect. Apart from the original looping approach the extraction methods of the resonant RV alternator R and D started with the addition of diodes driven by opto SCR or FET circuit switching.

The following Resonance collection circuits from Phil and Ravio will be presented in chronological order. Much has evolved and been perfected since the first disclosures. The circuits will be presented from start to current to bring the reader up to ‘scratch’ from the beginning and enable him\her to follow the thinking behind the concepts. There have also been many improvements in inverters for use in these configurations. Currently recommended is Dans and Raivos SG inverter.

1St resonance collection Circuit

The circuit works by cascading the energy away from the resonance side but keeping cap1 always in a half charged state to minimize a current draw from the resonance. After the first one or two hits from the resonance side cap1 is passed the basic 90deg phase shift and the continuing collections are more voltage potential without any damage to the resonance.

While cap1 is being charged cap2 is being discharged. When cap1 is fully charged it dumps into cap2. Because the voltage is balanced and halved when cap1 does the dump, cap1 is ready to take voltage potential where the current phase shifts is much less.

Laymen’s by peter

The diode bridge at the input is to turn the AC into pulsating DC. On the RH side - battery, 22v zenner and NPN FET are to provide power to run the one shot and flip flop circuits, and so can be disregarded as far as operation. The 15 volt zenner and other close by one are to set the trigger point when the one shot fires. It will produce a fixed width pulse  to drive the top and bottom FET as the input voltage rises past the set point. The middle FET is turned on when the other two are off by the flip flop circuit. The idea is to change the caps (1 and 2) separately, via the FET switches, then feed the power to the load in pulses.

Circuit parameters and values

On the Mosfet with the 22 volt Zener diode.  The mosfet gates require a 20 volt charge to fully switch on. If the circuit is running off a 12volt battery the mosfets will over heat, unless a pump charge circuit is used to lift the main rail up.  So the intention is to tap into some of the resonance side for the voltage lift so all will work as it should and reduce the smoke.

The two caps in parallel that will half the cap volts, and the cap energy goes as the square of the voltage. 2 Batteries is really the only way it will ever happen, and the trick is to keep the batteries at a particular voltage level where there resistance is fairly close to a constant. Also just by oscillating between both batteries like 500 times a second or faster so they are being charged and discharged within a flash, works very well.

You will need the 2 battery banks for its operation to partly loop the sequence. The added gains will be coming from the original motor and you can do what you like with the generator side. I decided to design the circuit as a system where you can drive any type of load and you can select any frequency for the Transformer.

Dans perspective

This circuit can be seen as a variant of hectors diode plug. I redrew the circuit for my clarity reasons (as I used to draw according to a certain standards), but not changed the circuit itself (I hope).See below I think the square wave of 1kHz as it mentions, is arbitrarily, as the best resonance of the coil should be sort after. The good thing about this circuit, is that the pulses on Q1..3 are in sync with the coil resonance.C1 & C2 is only discharged to 50%. One thing though, I believe for tuning purposes, that the pulse width should be made adjustable

A further note from Phil

There is something that some may not understand when using Mosfets specifications.  If a Mosfet has specifications stating that it is 200volt and 100AMP, the 100AMP rating is only when operating at 10volts. This also is when it is operating in a continuous ON state.  If it is being used in a pulsing situation there is another specification that states what current it can handle. This other rating is normally 2 or 3 times the continuous current rating but still only at 10volts.  So in the real world our 200volt mosfet if it was driving near this high voltage, can only handle about 2.5AMPS and this is pushing it very hard. In just about all FET models, the body diode has the same voltage and current rating as when in the on state, and no other diodes are normally necessary for added protection. Also it is normally a cheaper and better solution too use FET's where a diode is required. Phil has since perfected this concept.