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Overunity Machines Forum



Selfrunning Free Energy devices up to 5 KW from Tariel Kapanadze

Started by Pirate88179, June 27, 2009, 04:41:28 AM

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0 Members and 178 Guests are viewing this topic.

Goat

@ Woopy

I think that what romerouk was referring to with the second MOT was to connect the one wire of the first MOT's secondary side to the secondary side of the second MOT in series, then you can use the output of the second MOT's primary.....your diagram shows the second MOT hooked up in parallel not in series.

"For people having one extra MOT try connecting the output from first MOT to  the second one (high voltage part) in series, then the capacitor, then the SG."

Regards,
Paul

vrand

Quote from: Goat on June 17, 2010, 08:45:01 AM
@ Woopy

I think that what Romeo was referring to with the second MOT was to connect the one wire of the first MOT's secondary side to the secondary side of the second MOT in series, then you can use the output of the second MOT's primary.....your diagram shows the second MOT hooked up in parallel not in series.

"For people having one extra MOT try connecting the output from first MOT to  the second one (high voltage part) in series, then the capacitor, then the SG."

Regards,
Paul

The 2nd MOT in series to the 1st MOT will create Inductive reactance:

INDUCTIVE REACTANCE

When the current flowing through an inductor continuously reverses itself, as in the case of an ac source, the inertia effect of the cemf is greater than with dc. The greater the amount of inductance (L), the greater the opposition from this inertia effect. Also, the faster the reversal of current, the greater this inertial opposition. This opposing force which an inductor presents to the FLOW of alternating current cannot be called resistance, since it is not the result of friction within a conductor. The name given to it is INDUCTIVE REACTANCE because it is the "reaction" of the inductor to the changing value of alternating current. Inductive reactance is measured in ohms and its symbol is XL.

As you know, the induced voltage in a conductor is proportional to the rate at which magnetic lines of force cut the conductor. The greater the rate (the higher the frequency), the greater the cemf. Also, the induced voltage increases with an increase in inductance; the more ampere-turns, the greater the cemf. Reactance, then, increases with an increase of frequency and with an increase of inductance. The formula for inductive reactance is as follows:

http://www.tpub.com/neets/book2/4a.htm

woopy

thanks to all

What i need to know as soon as possible is :

in the diagram named "first idea A",  can i use a microwave cap of 0.1 uf 2100 volts as it is shown in the diagram ?

yes or no

i will go step by step so the first step is the cap  than the SG and only than the second MOT and other tuning. to see the difference.

thanks
Laurent

romerouk

Quote from: woopy on June 17, 2010, 09:13:37 AM
thanks to all

What i need to know as soon as possible is :

in the diagram named "first idea A",  can i use a microwave cap of 0.1 uf 2100 volts as it is shown in the diagram ?

yes or no

i will go step by step so the first step is the cap  than the SG and only than the second MOT and other tuning. to see the difference.

thanks
Laurent
a 2.100v capacitor is not good enough, try using 2 in series (remember using capacitors in series will reduce the value to half) to be able to handle aroud 4000v
#I am posting few diagrams with what I am working on regarding Kapanadze high voltage input.

romerouk

Here are the diagrams that I am using currently. Don't ask me about the MOT2 output as i am not going to talk about yet.