TSSP: List Archives

From: "Terrell W. Fritz"
Date: Fri, 25 May 2001 15:41:12 -0600
Subject: Re: [TSSP] Genetic optimisation

Hi Boris,

I remember Marco's coil as having a power supply problem that may have
affected this:

http://www.pupman.com/listarchives/2000/November/msg00117.html

I forget the details but that may have affected his toroid breaking out at
that time.  Marco's system is very good for this since his is so well
controlled.  I have his system running now so I'll report back.  I may have
to use a fairly large grid size and adjust things to get good resolution at
the toroid surface...

Catching up on mail now ;-))

Cheers,

	Terry




At 11:50 AM 5/23/2001 -0700, you wrote:
>
>Hi Paul,All,
>
>> Looks like 26kV/cm is the figure to work with at
>> normal TC frequencies,
>>  - comes as some relief that the value is not
>> severely frequency
>> dependent, things would be tricky if so!
>---
>Surely,~26-28KV/cm critical surface field would be all
>right to assume for TC freqs (and standard
>atm.conditions)
>Definitely,if such field appears for a certain time
>,it will get  show to start happening per see.
>But,what counts the most here is one thing:TIME...
>By this I don't mean just time of TC waveform
>exceeding this treshold ,but also time pauses between
>2 primary condensers bangs-->in other words some
>depedence on BPS (belive it or not!).
>John Freau experiments with smooth toroids are very
>valuable when we speak of this matter.
>He has noticed smaller bang size (innital cap energy)
>needed for visual spark breakout with higher BPS rate
>than with lower BPS rate.
>Few months ago,I contacted with M.Denicolai and he
>said he would make controled experiments on his thor
>in order to investigate such phenomenon this summer .
>
>Something else you should know as well.With about 400
>KV peak voltage on his coil Marco was unable to get
>breakout of his 20*150 cm smooth toroid.
>Only with Ep~10 J he started to observe first faint
>streamers coming from the terminal.
>Question improved E-Tesla program should answer to:
>What max. toroid surface field corresponds to 400 KV
>voltage on THOR secondary?    
>----
>
>
>> 
>> If I've understood things right, the leader
>> formation begins and
>> continues as long as this gradient can be maintained
>> just ahead of the
>> leader. I guess the significant threshold involves
>> meeting this value at
>> the surface of the smooth toroid and once a leader
>> begins to form, its
>> sharp point will then ensure that the leader forms
>> rapidly for quite
>> some distance - even though the 'background' field
>> from the
>> topload would, by itself, fall below the 26kV/cm
>> threshold only a little
>> way from the surface. Subject to the toroid having
>> enough charge
>> available to support that formation. What stops the
>> leader formation?
>> I guess either it hits earth or it runs out of
>> charge - the toroid is 
>> depleted and the 26kV/cm cannot be maintained at the
>> tip? So a big 
>> toroid would be reluctant to break out (modest
>> surface gradient), but 
>> it would throw a long streamer as soon as it did
>> (lots of charge 
>> available)?
>> 
>> I'm afraid I've got some more questions!
>> 
>> > A long spark (>6 cm) is characterized by multiple
>> avalanches in an
>> > evolutionary sequence: streamer flash(es) -->
>> leader propagation
>> > (fed by groups of streamers) --> spark (if leader
>> > bridges the gap).
>> 
>> Can we assume that this whole sequence takes place
>> in a timescale short
>> compared with an RF cycle - I suppose thats so
>> because if not there 
>> would be a bigger frequency dependence?
>---
>I think we can,althought some scopings on 250 Khz+
>coils I saw in past ,displayed not so small
>differences.
>--- 
>
>> 
>> When the HT falls away, do things recombine and
>> settle down sufficiently
>> that on the next half cycle there is no 'memory' of
>> the previous half
>> cycle?
>> 
>> Ultimately what I'm fishing around for is some
>> confidence that some
>> acceptable and realistic account can be taken of the
>> breakout
>> thresholds, otherwise attempts at non-linear time
>> domain modeling will
>> founder on that point.  I feel as though we are on
>> top of the technical
>> matter of computing the response and now, quite
>> suddenly it seems, we
>> are up against this more difficult problem of
>> finding a load conductance
>> function which provides an acceptable summary
>> description of the
>> breakout dynamics. 
>> 
>> If I've got things right, then Terry should be able
>> to calculate quite
>> easily the top voltage at which streamers should
>> suddenly start to form,
>> and we might also be able to calculate an estimate
>> of streamer length
>> too (as a function of topvolts). Given those two
>> separate figures (or
>> functions) we would then have the choice of
>> optimising for max topvolts
>> or max streamer length, using the same genetic
>> software but with two
>> different merit functions.
>> 
>> Cheers,
>> --
>> Paul Nicholson,
>> Manchester, UK.
>> --
>
>Regards,
>boris
>
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Maintainer Paul Nicholson, paul@abelian.demon.co.uk.