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Re: El Supremo
Original poster: "K. C. Herrick by way of Terry Fritz <twftesla-at-qwest-dot-net>" <kchdlh-at-juno-dot-com>
Terry (& all)-
I'll interpose comments (and I wish that my received emails did not
include a whole lot of superfluous "carriage returns"; does everyone
suffer that?)...
On Thu, 12 Sep 2002 17:40:10 -0600 "Tesla list" <tesla-at-pupman-dot-com>
writes:
> Original poster: "Terry Fritz" <twftesla-at-qwest-dot-net>
>
> Hi Ken,
>
> I was looking at this all afternoon!! :-))))
>
> At 09:09 AM 9/12/2002 -0700, you wrote:
> >Terry Fritz's groundbreaking work with the OLTC has given me pause
> to
> >think about my own design and how it might be improved. Also
> constantly
> >in my mind is an appreciation of the ratio of my MOSFET failures to
> his
> >IGBT failures: it's infinity, not to put too fine a point on it,
> since
> >dozens upon dozens have failed for me and none have failed for
> him.
>
> The big factor there is that I am switching at only 120 Hz. No high
> speed
> switching stuff to worry about at all.
>
> >
> >Terry's 1-turn-primary design is what I had had in mind in the
> first
> >place, but my MOSFETs would not drive 1 turn and IGBTs back-then
> seemed
> >too slow. But now, I see a way to combine Terry's notion and mine.
> I
> >call it, perhaps with some want of humility, El Supremo. With
> Terry's
> >indulgence you can find its conceptual schematic at
> >Http://hot-streamer-dot-com/temp/tch2.gif. See also the accompanying
> >http://hot-streamer-dot-com/temp/tch2drv.
>
> The second URL really should have been this but I fixed it so most
> browsers
> would still work.
Yeah, I goofed there; hope everyone got around that.
>
> http://hot-streamer-dot-com/temp/tch2drv.gif
>
> >
> >Referring to TCH2, all IGBT "1"s conduct during one half-cycle and
> then
> >all "2"s conduct during the alternate half-cycle. If you follow
> the
> >current paths you will find that the four quadrants of capacitors
> become
> >connected in a "daisy chain" around the primary loop in
> alternating
> >polarities, thus establishing the requisite alternating magnetic
> field
> >perpendicular to the image.
> >Each set of IGBTs is driven by a crossover-controlling circuit like
> that
> >of TCH2DRV.
>
> The big thing "I" see here is that with only a minor rearrangement,
> you
> have 2400 volts instead of 600 driving the secondary in sort of a
> Marx
> configuration. That allows higher frequencies (far less secondary
> loss),
> and lower loss in the primary!!! Just what my OLTC needs!!!!
> :-))))
You lose me here. Do you mean, charge each of the 4 sections to 600 V
instead of 150? No problem there, conceptually. But how does that allow
for higher frequency?
>
> "I" don't see the great need to switch two circuits at the Fo
> frequency for
> my OLTC type of coil.
I assume here you mean, switching actively for each half-cycle rather
than passively, thru the diode, as you currently do. No, you wouldn't do
that for the OLTC-type--but El Supremo would have to incorporate that
since there's no primary resonance to set up the cycling. The capacitors
are just discharging dc-wise.
>
> >
> >Note that, during each brief interval between half cycles when no
> IGBTs
> >are conducting, the "inductive kick" of the primary loop will
> become
> >clamped, regardless of its polarity, by the "fast diodes", as
> coupled via
> >the loop capacitors. No transistor will ever see any voltage
> greater
> >than twice a capacitor voltage.
>
> That does work very well!! The IGBT reverse diodes work perfectly!
Yes, if they're built in, so much the better...
>
> >
> >Now here is where a major difference with my present design comes
> in:
> >
> >The fundamental difference between sstc's and spark-gap tc's is
> that the
> >former generates its spark by application of a constant-amplitude
> burst
> >of excitation whereas the latter generates an
> exponentially-diminishing
> >amplitude of excitation. This means that by far the greatest
> amount of
> >instantaneous energy going into the spark is delivered, in a
> spark-gap
> >system, during the first few cycles of excitation. It does not
> escape
> >notice that, given the same mains input-power, a spark-gap coil
> will
> >produce significantly longer sparks than a sstc--even given the
> >relatively large loss of power in the spark gap. So, it is very
> likely
> >to be concluded that what's wanted is to cram as much power as
> possible
> >into those first few cycles.
>
> Remember the "peak power"! A sstc runs 100% of the time at 1X the
> power.
Well..not mine: Mine is "disruptive" just like yours. So many ms
sparking, so many ms just sitting there.
> A disruptive coil runs 5% of the time at 20X the power. 20Kv at 500
> amps
> is 1,000,000 watts of power into the streamer! You be it "jumps"
> ;-)) Do
> note the remarkable streamer length increases using the "staccato
> mode" in
> CW coils. A very interesting affect that is due to electrostatics
> but may
> be very important to us and streamer length. We are nearing the
> point of
> having very good control over such unexplored factors.
Since both my coil and someone else's spark-gap coil are "disruptive",
and they sit side-by-side, so to speak, and draw much the same power from
the mains, and yet--the other guy's sparks are 30% longer...I have to
conclude that that has something to do with the shape of the power
impulse put into the secondary. That's why I conclude it's best to
emulate a spark-gap coil, in putting by far the most of the power of each
spark into the first few cycles of that spark's excitation.
>
> >
> >So what I propose with TCH2 is that the capacitances be markedly
> smaller
> >that what I have in my present design. In fact, they are to be
> small
> >enough to give the desired rate of exponential decline in voltage
> during
> >each spark event. Note that the current in all the capacitors is
> >unifirectional, not ac and that the primary is still untuned. The
> >capacitor voltages just decline during the spark event, they do
> not
> >change polarity. And since the IGBTs are to be driven from an
> external
> >signal source, that source can either be tuned at will to match
> the
> >secondary's Fr or it may readily be derived directly as a function
> of the
> >secondary's return-current, as I do presently, to make the system
> >instantaneously self-tuned to the secondary's Fr.
>
> Self tuning and frequency control is really nice. But the logistics
> of
> making it work scare "me". I'll stick with the plain simple 120BPS
> tuned
> primary ;-))
But "120 BPS" and "tuning" mean different things: 120 BPS is the
repetition rate of the "tuned" burst of sine waves that excites the
secondary. What's tuned is the frequency of the pulse-burst, & not the
120 BPS--right? That's where it's really handy to have that always
"tuned" to the secondary's Fr. Whenever that secondary is moved to & fro
with respect to grounds, its Fr changes, of course, by a substantial
amount.
>
> >
> >Most importantly, this scheme acts to completely separate the
> function of
> >frequency-determination from the function of spark-energy storage.
>
> >Change the frequency? Just do it: the energy available to create a
> spark
> >won't change. Increase or decrease the primary's time-constant?
> Just do
> >it: the frequency won't change.
> >
> >And notice one more interesting thing: I show the capacitors as
> being
> >connected to the primary buses all along their lengths. I think
> that it
> >doesn't matter where they are connected since a) their current is
> >unidirectional and b) the current in each of the buses is
> unidirectional.
> > There exists the same length and locus of conductor regardless of
> where
> >a capacitor is connected. The advantage is that a large number of
> small
> >capacitors may be closely attached to the conductors, both
> maximizing
> >their overall current-carrying capability and minimizing their
> lead
> >inductances and the overall ESR. Also, it's a handy place to put
> >them--all around the periphery of the primary.
>
> I worry a little about using caps as a primary inductor element
> directly.
> Not sure what kinds of odd electrostatics goes on there. Streamer
> hits to
> a primary cap (optimistic ;-)) would be a bad thing.
Oh, I wouldn't worry about that at all. Nothing but good old C, L & R
inside those capacitors! And as to streamer-hits, with the cap's on the
outside of the primary conductors, the hits will go to the copper rather
than to the capacitors.
>
> >I envision two
> >1/2"-diameter copper pipes for each segment, spaced vertically
> perhaps
> >1/4" apart and with the capacitors' leads soldered to their outer
> >peripheries. Easy to assemble, easy to change the capacitors.
Now, I think more like 1": substantially lower inductance.
> >
> >I show 4 primary segments in TCH2 but could be any even quantity.
>
>
> There is a practical limit. Probably more based on how much
> voltage/power
> an IGBT can handle and what kinds of faults it may see. Perhaps a
> physical
> limit too. Just have to work the numbers...
>
> >Also,
> >the capacitors could be charged in various ways, for example from
> >current-regulating supplies as in my present design or resonantly
> as in
> >Terry's OLTC design.
>
> They can be "one" supply :-))) Think Marx generator. Simple
> resistors can
> isolate the section during firing since say 5 ohms is trivial to a
> 0.01 ohm
> primary loop. All the current will ignore the 5 ohms...
That's right.
>
> >
> >Current-sharing amongst the paralleled IGBTs should not be a
> problem:
>
> Watch out for that one!! Just a little inductance or a late turn on
> and
> boom! This is especially true when running them at 3X their peak
> rating
> :o))) Try to think about using the cap impedances to force current
> sharing
> like the OLTC. That works great!!
You may well be right. But I puzzled a long time as to how I could use
separate capacitors for each transistor & couldn't see how to do it.
>
> >A
> >very small emitter resistor developing perhaps 0.2V at peak
> emitter
> >current should suffice to steer current away from the stronger
> >transistors into the paralleled weaker ones.
>
> Yips!! No!! That 0.2 ohms is an enormous power drain for a
> disruptive
> coil! Think of what it does to the primary Q. If you have say 0.5
> ohms of
> primary resistance in a 20Arms primary circuit that is 200 watts of
> real
> power!! I would never consider adding any resistance in the
> primary!
No!, no! Not 0.2 ohms but 0.2 volts: that's all you'd need to persuade
the other paralleled transistors to take up the load, with their
conducting Vc-e's of maybe 3 V or so.
>
> >Such a resistor might well
> >consist merely of the lead connecting each IGBT's emitter to the
> common
> >point.
>
> Watch inductances! 13nH is small until you have 200 amps at 100kHz.
> Then
> you have 1.6 volts (reactive) which is enough to cause problems.
Yeah, very likely. Murphy...
> That is
> just what goes on "inside" the IGBT case let along what we solder to
> it next...
>
> >Further, avalanche-breakdown should never be a problem since no
> >transistor can see any voltage greater than twice a capacitor
> voltage
> >under any condition.
>
> TVS transorbes are wonderful things too just to be really sure!!
Try it first without?...
>
> >
> >And finally, this is a low-voltage design. I remember, when I was
> a kid,
> >that the president of the ARRL was killed by his ham apparatus'
> high
> >voltage. That's always stuck in my mind.
>
> Low voltage is wonderful. All kinds of conventional tricks can be
> used
> that are not available to us at 20kV!! However, if we get higher
> (2400V)
> firing voltages, things get a little more complex.
Yeah, you're just as dead from 2400V--but not quite as dead as from 150V.
>
> >
> >It seems to me that this idea has great potential. I hope I will
> >personally have the energy to look further into it & build it and I
> urge
> >others to contemplate doing so. Or else...to contemplate telling
> me that
> >it won't work.
>
> Such a system for the OLTC looks very promising!!!! Switching at
> only
> 120BPS still but using your four section system could solve many
> problems!!!
>
> Cheers,
>
> Terry
Ken