Kapanadze Cousin - DALLY FREE ENERGY

[Hoppy]

I think that Hoppy was objecting to the insufficient power to run the ATX PSU when supplied by L4 or insufficient voltage due to L4/L1 turn ratio (83/475=~1/6). Even if the unloaded L4 voltage was sufficient to run the ATX PSU then most likely the power input provided to the cylindrical coil L1-4 (by transformer Tr2), was insufficient to maintain this voltage when loaded with the ATX PSU.

His objection has merit if the transformer Tr2 (driven by TL494) is the only source of power to L4.

Hoppy's objection has no merit if there is power gain between L1 and L4 because of some undiscovered process stimulated by the nanopulses in L3 and the oscillations of the LC tank composed of L2 & C?.

IMHO this above energy gaining process can be stimulated in a Gain Medium such as ferrite, brass, or copper tubes/rings, but not in the Vinyl glue dispenser tube or air.

Yes, that is what I was getting at because we have to assume that Dally's L4 coil powered the PSU using the coil winding ratio as worked out from his set of photos. clearly a lot more turns will increase the voltages but we also need a couple of amps or so to run the PSU from somewhere. The best I can do is 17V DC on L4, dropping to 13.8V with a 1 Amp load, which is a long way off 150V!

I ran up my replication today without the AT PSU and powered the circuit form my bench PSU. Pulses from the nano pulser applied to the co-ax had no affect on the coil output voltages at any setting on the pot. I also tried various different cap values for tuning L2 around resonance. Anyway, I'm now going to leave things until I get back to the bench in a weeks time.

Regards
Hoppy

[verpies]

After posting the last message about nanopulse generation with DSR diodes, I received so many private messages that I am posting the article below.

Please check the wording for any errors or issues that are not clear and PM me if you find any, as I would like to polish it up for publication.

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The current waveform applied to the DSR diode can be generated by many different techniques, such as: a pulse transformer with saturable core, inductive flyback pulse, dual switch scheme, etc…

The DSR diode pulse generator depicted in Fig. 1 consists of two circuits with a fast power transistor Q1 (e.g.: MOSFET or IGBT, GaAs BJT, etc…) between them.
The first circuit is composed of inductive energy storage L1 and the second circuit is composed of a capacitive storage C2, inductive storage L2 and DSR Diode D1 (connected in parallel with the load resistor R1). Note that L2, C2, Q1 and D1/R1 form a series RLC circuit. Hereafter this circuit will be referred to as simply: “the series RLC circuit”. 
The capacitor C1 is used to stabilize the supply voltage and decrease the effective internal resistance of the power supply at high frequencies.

Before the impulse generation begins, the transistor Q1 is not conducting (the circuit is open between the drain and source terminals) and the capacitor C2 is charged up to the power supply voltage via the load resistor R1.

To begin nanopulse generation, a short pulse is applied to the gate of Q1 causing it to start conducting.
As soon as the transistor Q1 starts conducting, two events take place:
1) The capacitor C2 discharges through the forward conduction of D1 and
2) the inductances L2 & L1 start accumulating energy (the currents through them increase).

The current through L2 is inherently periodic if the series LCR circuit, formed by L2, C2, Q1_RDS-ON and D1/R1, is underdamped, that is: its total resistance is less than 2(C/L)^0.5. The period of this oscillation is equal to 1/( 1/LC - R²/4L² )^0.5.

After approximately one-half of this oscillation period (after interval T₁), the transistor Q1 stops conducting.  See Fig.2.
During the interval T₁ the D1 diode was conducting forward and charge was injected into its P-N junction.
For the manifestation of the DSR effect it is very important that the T₁ interval is short enough (in the hundreds of ns) to not allow the injected charge to reach the other side of the P-N junction.

During the T₁ interval, the periodic current through the series LCR circuit has reached its peak and and decreased back to zero. At the beginning of the interval T₂ the current through D1 begins to reverse its direction due to the transient oscillation of the series RLC circuit, effectively causing D1 to conduct in reverse and gradually deplete the charge injected into its P-N junction during T₁.

From the beginning of interval T₂ the current flowing through L1 joins with current flowing through L2, D1, C1, C2 and R1. As soon as the charge injected into the P-N junction of D1 decreases to zero, the DSR diode abruptly stops conducting. This happens at the end of interval T₂.

Because this abrupt interruption happens when non-zero reverse (negative) current flows through D1, L1, L2, C1, C2 and R1, a high voltage pulse appears across the D1 terminals due to the self-induction effect.
The rise time of this pulse is determined by inductance L1 and L2 and the reverse capacitance of D1.
The energy accumulated in L1 from the beginning of Q1’s conduction and in L2 during the D1’s reverse conduction (T₂) is converted into a high electric potential appearing on the D1’s reverse capacitance.

The peak power of this pulse is approximately equal to the product of the interrupted current magnitude, determined by the impedances the associated components, and the reverse capacitance of the DSR diode D1.

In order to maximize the DSR diode effect, the forward current through the diode should be lower and of longer duration, yet the reverse current should be higher and of shorter duration.
If forward and reverse current waveforms are the same then the DSR diode stops conducting when the current through the diode is equal to zero and the DSR effect disappears.
An optimal operating point for the DSR effect occurs when the DSR diode stops conducting at the peak of its reverse current.

P.S.
L1 and L2 should be air core inductors wound with a thick wire and positioned perpendicularly and away from each other.
The capacitors should be designed for RF pulse operation.  The leads of all components should be soldered as short as possible.

[Vortex1]

Great job on that verpies, very much appreciated.

BTW a lot of the literature talks of using thyristors (SCR's) as SRD's.

I was wondering about that red device again since it is 3 terminal.

[d3x0r]

Great job on that verpies, very much appreciated.

BTW a lot of the literature talks of using thyristors (SCR's) as SRD's.

I was wondering about that red device again since it is 3 terminal.

One of those is in this replication....


http://www.youtube.com/watch?v=yvCzuC8U8EY


This post has a nice close-up of this guy's replication with the KT926 and KD203A's


http://realstrannik.ru/forum/44-freeenergylt/82460-novyj-variant-ustanovki-free-energy-dally.html?limit=18&start=1152#86168


I know someone, somewhere posted a picture of a KT926, but I can't find that; maybe it was in the kapanadze thread here - the Dally stuff started at page 929 until about 945(?)...

[T-1000]

I think Ganzha is probably right and we are looking at a fake.

Nope, he's not and you should see wires leading to startup battery in http://www.youtube.com/watch?v=QHBEHOOsxT4#t=0h34m50s Later that battery is disconnected.

Ones who want see faked device all the time will always find mehods to "prove" it...

P.S> Ganza's posts are just a waste of time in my opinion and I will ignore them from now. First he attacked our NMR yoke device then insulted many times trying to get people fighting instead of cooperating then insults in regards to Dally device. The forum Troll in other words ( http://curezone.com/forums/troll.asp )