The actual phenomenon encountered is probably a plasma production by dielectric breakdown across the gap followed by trans-plasma conductance. The prediction of the rate of plasma production and resulting change of concentration of plasma (dC/dt) and the associated decrease in pressure of air and it's dielectric effect (dP/dt) should be modelable. See attached. Note discharge resistance.Subject: Re: PSpice modeling of spark gaps Resent-Date: Thu, 12 Nov 1998 09:07:57 -0700 Resent-From: tesla-at-pupman-dot-com Date: Thu, 12 Nov 1998 08:27:09 -0700 From: Tesla ListTo: tesla-at-pupman-dot-com Original Poster: "Barton B. Anderson" Hi Malcolm, Tesla List wrote: > Original Poster: "Malcolm Watts" > > Hi Bart, > > Closest I've come has been scoping primaries and deducing the basic > characteristics from the waveforms, then applying a bit of math to it > to reach some interesting conclusions regarding Q etc. I have also > tried using a bank of MOSFETs in place of the gap to investigate > quench issues and resonator action. Additionally, after forming and > opinion as to the nature of the real gap model, I did setup a > benchtop LC circuit and stuck in both back-to-back zeners and anti- > parallel diodes (low drop relative to the peak cap voltage). The > zeners were unrepresentative at the low voltages I was working with > but the diodes did a nice job *provided that the operating point was > carefully picked*. I found that I could obtain log, linear and > antilog responses depending on which circuit values I used so it pays > to be careful when using diodes of any sort as a substitute for the > real thing. > The most amazing finding the math revealed was that Q for a > tuned circuit with a gap in it couldn't be quantified as a fixed > value the way it can if there is normal resistance only. The math > showed that Q climbed with voltage and absolute losses increased with > current. The reason for this is that Vgap is not proportional to Igap. > Neither voltage nor current is a fixed quantity but continuously > varying in normal circuit operation. > > Malcolm Yes, the gap is complex and difficult to model these details. I remember when you posted your results sometime ago. It is interesting. I'm not sure I can grasp Vgap not being proportional to Igap. Even with varying capacitive and/or inductive loading in the gap, V and I should remain proportional, unless there's a new physical law I don't know about. If Q climbed with voltage then it appears to me the "gap" reacts capacitively in nature and the gap capacitance changes with volts/time as well as with varying current. Wouldn't Q then follow Vgap? My thinking here is if Cgap = Igap / (dv/dt) = Q/V. Sorry I didn't reply sooner, I've been in the garage the past couple nights building a new spark gap. Bart
http://iyl.ee.titech.ac.jp/res-e97/UV-e.html
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- To: tesla-at-pupman-dot-com
- Subject: Re: PSpice modeling of spark gaps
- From: Tesla List <tesla-at-pupman-dot-com>
- Date: Thu, 12 Nov 1998 08:27:09 -0700
- Resent-Date: Thu, 12 Nov 1998 09:07:57 -0700
- Resent-From: tesla-at-pupman-dot-com
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Original Poster: "Barton B. Anderson" <mopar-at-uswest-dot-net> Hi Malcolm, Tesla List wrote: > Original Poster: "Malcolm Watts" <MALCOLM-at-directorate.wnp.ac.nz> > > Hi Bart, > > Closest I've come has been scoping primaries and deducing the basic > characteristics from the waveforms, then applying a bit of math to it > to reach some interesting conclusions regarding Q etc. I have also > tried using a bank of MOSFETs in place of the gap to investigate > quench issues and resonator action. Additionally, after forming and > opinion as to the nature of the real gap model, I did setup a > benchtop LC circuit and stuck in both back-to-back zeners and anti- > parallel diodes (low drop relative to the peak cap voltage). The > zeners were unrepresentative at the low voltages I was working with > but the diodes did a nice job *provided that the operating point was > carefully picked*. I found that I could obtain log, linear and > antilog responses depending on which circuit values I used so it pays > to be careful when using diodes of any sort as a substitute for the > real thing. > The most amazing finding the math revealed was that Q for a > tuned circuit with a gap in it couldn't be quantified as a fixed > value the way it can if there is normal resistance only. The math > showed that Q climbed with voltage and absolute losses increased with > current. The reason for this is that Vgap is not proportional to Igap. > Neither voltage nor current is a fixed quantity but continuously > varying in normal circuit operation. > > Malcolm Yes, the gap is complex and difficult to model these details. I remember when you posted your results sometime ago. It is interesting. I'm not sure I can grasp Vgap not being proportional to Igap. Even with varying capacitive and/or inductive loading in the gap, V and I should remain proportional, unless there's a new physical law I don't know about. If Q climbed with voltage then it appears to me the "gap" reacts capacitively in nature and the gap capacitance changes with volts/time as well as with varying current. Wouldn't Q then follow Vgap? My thinking here is if Cgap = Igap / (dv/dt) = Q/V. Sorry I didn't reply sooner, I've been in the garage the past couple nights building a new spark gap. Bart
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