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Pri circuit effective resistance.



Original poster: "resonance" <resonance@xxxxxxxxxxxx>



Did the 0.16 value include your total primary circuit or just the value thru the SISG switching device?

Regarding the effective resistance in the pri circuit, 3 Ohms vs 0.16 Ohms is a tremendous difference as with regards to performance.

Would you suspect also that the DRSSTC IGBT switched coils are also seeing effective resistance in this range? Anyone on the list like Steve W. actually measured this value?

This would certainly explain why the DRSSTC's only require approx 400 - 500 Watts per foot of spark output vs the usual 1 kW for classic coils.

Dr. Resonance


Although spark length is really directly related to power, not potential, it does require a high potential to begin the ionization process, so the basic idea is to apply the equation for potential in an air coil inductor:

It seems to require "both" power "and" potential for the optimal sparks. There are very high voltage coils that perform poorly and there are very powerful coils that perform poorly. But high voltage powerful coils do very well. This problem shows in ScanTesla's streamer length predictions if one uses parameters that are not "typical". The program does do it fairly well now in most cases by combining power and potential together to come up with leader length and strike distance. It is not perfect yet or anything, but there are no giant obvious errors now. I also have plenty of fudge factors to fix the remaining small errors :o))

.......

The rate change of current, dI/dt really depends on a number of efficiency factors such as spark gap resistance, primary connection resistance, etc. We use 4 AWG welding cable with copper battery lugs for our primary connections (inside tygon tubing) and use 3/4 - 1 inch dia. copper pipes for our sparkgap thus keeping the switching (dI/dt) value high as possible in current and fast as possible in quenching time of the sparkgap). High current (the dI) and fast speed (the dt) is important.

From the old post at:

http://www.pupman.com/listarchives/2006/Aug/msg00201.html

At t~0:

dI(t)/dt = Vfire x SQRT(Cp / Lp) x 1 / SQRT(Cp x Lp) x COS(t / SQRT( Cp x LP))

If t ~~= 0 and with some simplification we get:

dI(t)/dt = Vfire / Lp

dI/dt is really almost totally "independent" of losses!!! What losses do is "eat up all the power" before it turns into streamers by destroying the primary system's "Q".

Qp = SQRT(Lp / Cp) / R

R (losses) kill primary "Q", not primary dI/dt.


It is very interesting to note that the Q numbers for the SISG PIRANHA are:

Qp = SQRT(15e-6 / 165e-9) / 0.16 = 59.6

However, if it used a conventional gap where R = 3.0 ohms:

Qp = SQRT(15e-6 / 165e-9) / 3 = 3.17

It would not even run "at all" with conventional spark gaps!! Thus my warning to "don't even try" to use that topology without SISG spark gaps!!

http://drsstc.com/~piranha/PIRANHA/PIRANHA.pdf
....

Assuming the average coil's efficiency around 70%, then the sec voltage equation becomes:

Vsec  =  Vpri x 70% x SQR (Lsec/Lpri)

I've used antenna current x field measuring systems developed by Terry Fritz (our super-duper moderator) and this equation is very close ---
usually within a few percent so it really does work.

Glad to know that number works for someone else too!!!! It is hard to get independent verification of such things!

...

Cheers,

        Terry



Happy coiling,

Dr. Resonance