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It seems to work fine for conventional, SISG, and DRSSTC coils now. I included examples of all of them. The streamer load model is in the C file (plain text), but the meat looks like this:
Pretty simple now. I got the simulations and all done and added now so the constants are accurate. The program also has goal type 3 now to search for the best streamer length. Dwell time can also be used for conventional coil quench time too. The arcs to ground seem to work well now and match the scope. So, finally, the program seems to be doing its master's bidding
The default input file in the ZIP is for Dan's new DRSSTC-III. I was not sure for the toroid diameter and maybe a few of the inputs, but they are probably close. The program gave this:
================ ScanTesla V-7.62 June 4, 2006 Terry Fritz Goal = 4.180500e+001 Maximum Leader Length Model Number = 940 Goal Number = 125 Cprimary = 1.100000e-007 Lprimary = 9.100000e-006 Rprimary = 1.000000e-001 Coupling = 0.182500 Csecondary = 2.099000e-011 Lsecondary = 4.387000e-002 Rsecondary = 3.850000e+002 Cload = 6.300833e-012 Rload = 2.200000e+005 BPS = 120.000000 Dwell (T1) Time = 6.800000e-005 Ilprimay Maximum = 560.892753 ICprimary RMS (Arms) = 22.307666 ILsecondary RMS (Arms) = 0.391537 VCprimary Maximum = -5120.878882 VCsecondary Maximum = -416110.197722 Coil Power = 328.820961 Primary Bang Energy = 2.740175 Load Power = 220.028924 Load Bang Energy = 1.833574 Leader Length (in) = 41.804996 Streamer Primary F0 = 159075.425254 Secondary F0 = 165855.582964 Load Energy Rise Time (uSec) = 50.600000
Registered Member #30
Joined: Fri Feb 03 2006, 10:52AM
Location: Glasgow, Scotland
Posts: 6706
Hi Terry,
Great stuff! I have some data that I captured from my own DRSSTC here: There is a DSO capture of the primary current during a ground strike. Is there any way we can get ScanTesla to model this and see how the simulated primary current matches up?
As regards probe bandwidth for capturing ground strikes: If the arc channel had very low resistance (which I believe it does) it would resonate like a metal antenna excited by a spark gap, much as in Hertz's original experiment. So, I imagine the ground current waveform would be a damped ringing whose frequency was such that the streamer was something like a quarter or a half wave long. That works out in the 50-100MHz range for the sizes of coils that most of us play with. The impedance of the connection to the ground target would affect this however.
Does your mutual inductance loop pick up i(t), or di/dt?
Great stuff! I have some data that I captured from my own DRSSTC here: There is a DSO capture of the primary current during a ground strike. Is there any way we can get ScanTesla to model this and see how the simulated primary current matches up?
The parameters I found for this situation did not match up right. I asked Steve if he still has the data on the coil measured. ScanTesla "should" be able to "do it" with the right input. If not, I will "fix it"
Does your mutual inductance loop pick up i(t), or di/dt?
That is a very good question??? I was just looking for "speed" data... All that "it" response data is unknown... I really have no idea other than the spark is "darn fast"!!!! and runs into the low thousands of amsps!!
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