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Overunity Machines Forum



ENERGY AMPLIFICATION

Started by Tito L. Oracion, February 06, 2009, 01:45:08 AM

Previous topic - Next topic

0 Members and 129 Guests are viewing this topic.

Cap-Z-ro

"...you don't even know where the walls of the box are."


I know enough to plainly see the box that encapsulates all of your text offerings.



Dave45

Well I havent built it so cant argue the point, just an idea.

It can be done and I will find it  ;)

Ionization- charge separation is the key

Separation of atmospheric charge is the answer

You dont have to separate matter the charge is there albeit neutral (joined) create stress, pull the charges apart.

Like our Russian brother said "separate - collect "





Bob Smith

Quote from: weizisky on May 04, 2014, 03:08:31 AM
it is better to learn fishing, to learn Tesla's or Bedini's devices.there are clear circuit diagrams there. if you know them well, you don't need to guess what Tito had said. otherwise, U just wast time here.

Tito's device is a simplyfied Tesla coil with the morden components: Z-DIODE AND TRIODE. or Z-diode
Weizisky
This is the conclusion I have come to - that the basic Bedini principle of collecting the inductive spike from a voltage pulse on a secondary is part of the equation. I believe the JFet (basically a solid state triode) will have a faster switching time than a mosfet. This is where I think Teets' Joule Thief clue comes in. It gives the pulse, and the RE (what some are calling bemf) backspike is harvested with a secondary.

Now, what to do with the harvested backspike from the secondary?  Does the zener figure in at this point?

Here's some interesting related info on the subject of the pyrazo device:
Quoteimagine now a feedback loop such as the one in the Pyrazo circuit. The signal will come through the primary of the transformer used for pulsing, then right at its peak in one direction, the current through the primary is interrupted, causing the fields to collapse, and causing a voltage spike in the secondary. This spike is then routed through the primary again in the other direction, which makes for an even more dramatic change in the primary's fields which is effectively a feedback loop of inductive kick.

This pulse is aligned with the signal so that it effectively pulls the signal with the same spike. Effectively, it is broadcasting a cancelling signal.

Without the feedback loop of inductive kick, it would be no more interesting than the coupled induction they are doing over at MIT.
Source:  http://www.energeticforum.com/renewable-energy/4550-pyrazo-circuit.html#post140393

The next stage, I believe is how to set up the caps to charge and discharge for a really big boom!  :D
Bob








Jeg

Hey guys
I need your help please. I am trying to find super ultrafast diodes with recovery time 20ns maximum with hv and high current characteristics. Do you have something in mind?
And one more thing. Many times I have read that spark gaps can work as diodes. But as I know during firing the oscillation goes back and forth through the gap. Is it something else that I don't know? What about the one I told you some posts above? I mean what if electrodes are different metals which have different position at the triboelectric list?

Tnks
Jeg

Bob Smith

Quote from: Jeg on May 04, 2014, 02:10:13 PM
Hey guys
I need your help please. I am trying to find super ultrafast diodes with recovery time 20ns maximum with hv and high current characteristics. Do you have something in mind?
And one more thing. Many times I have read that spark gaps can work as diodes. But as I know during firing the oscillation goes back and forth through the gap. Is it something else that I don't know? What about the one I told you some posts above? I mean what if electrodes are different metals which have different position at the triboelectric list?
Tnks
Jeg
Jeg, I figured a Schottky diode might help. I wasn't aware there are a new generation of Silicon Carbide Schottky diodes that seem even more reliable:
Quote
Schottky Diode
A Schottky diode recovers even faster than a silicon diode. Having a metal to silicon junction, it can switch at speeds up to tens of billions of times per second. While not suitable for every application, engineers use them in very high-frequency circuits.
Read more: http://www.ehow.com/facts_7505561_fast-recovery-diode.html#ixzz30mHA1hI6

The other main advantage of the Schottky diode is its fast recovery time--these diodes are extremely fast and exhibit little reverse recovery time. This is behind the Schottky diodes common use in switching regulator circuits and its popularity in high-frequency devices. The Schottky diode's fast recovery time can even eliminate the need for snubber circuits, which are commonly required with other types of fast rectifiers.

SiC Schottky Diodes
Silicone carbide (SiC) Schottky diodes are the newest innovation in Schottky diodes and boast a variety of improvements. This new type of diode has an even lower forward voltage loss than traditional Schottky diodes, and are easily paralleled for higher currents. SiC schottky diodes are also able to function at optimum performance levels regardless of temperature--something tradition Schottky diodes cannot do.
Read more: http://www.ehow.com/info_8187434_schottky-diodes.html#ixzz30mIFYYWa