Winfield said:
Bert Hickman wrote...
Starting at +7kV and swinging by 14kV takes the caps to -7kV,
isn't that a -7/12 = 58% voltage reversal? Or does the 20%
spec refer to rapid reverse-direction voltage swings rather
than reversed-voltage polarity?
The 20% spec actually refers to the maximum voltage swing during a rapid
discharge versus the rated DC voltage. In the above case we have
14kV/12kV = 1.16, or a 16% voltage reversal. See the following for more
info:
http://www.gaep.com/tech-bulletins/voltage-reversal.pdf
These can probably work to beyond-spec currents at the upper
end of their frequency range. You can test this by looping
multiple turns through the sensor, simulating "extremely-high"
currents. You can also parallel the sensor loop with alternate
wire paths, etc., to extend the range and you can calibrate the
setup at lower known currents to obtain the new ratio.
The Pearson 301X CT is rated at 50,000 amps (0.01 volts/amp, 50 ohm
output resistance, with a 3db cutoff at ~2 MHz). The 50 kA limit appears
to stem from the 500 volt maximum output voltage spec. However, another
Pearson App Note says that, if I terminate their CT's with a 50 ohm
load, I'll get half the output voltage/amp. I think this really means
that I can push the CT up to 100 kA without exceeding the 500 volt
output limit.
It'd also be valuable to grab the voltage waveforms, which is
easy to do with capacitive dividers. For example ~1 pF on the
HV side and 1000pF on the low side for a 1/1000 divider.
I do have a 60 kV Ross capacitive voltage divider. However, I'm
concerned about hooking this up to the storage scope because of the
possibility of getting substantial ground bounce when firing the system.
Measuring the current was is more attractive because of the fully
isolated measurement. Unfortunately, I don't have a battery powered
scope that I can float...
Appropriate shields are also necessary, since signal strays are
competing with the 1pF main path. The long-distance output coax
can be part of the 1000pF. You can complete the circuit with HV
resistors and zener clamps to protect the probe's opamp buffer
amplifier, which helps isolate an expensive scope. A trimpot can
be used for calibration at the output amp; a 10V cal signal gives
a 10mV output signal, enough for accurate scope readings during
the cal adjustment. I have made such dividers working to 25kV,
with a 100Hz to 10MHz bandwidth, and it shouldn't be too hard to
extend any of those parameters.
And, always remember to be afraid - very afraid - of the energy
stored in these caps. They will not give you any second chances.
=:^[
I'd like to ask a question about capacitor failure. Considering a
capacitor that's gradually degrading, I wonder if the final failure
can occur during charging, as opposed to discharge. This would mean
everyone should be far away behind shields whenever any paralleled
HV capacitor bank has a significant voltage on its caps.
It really depends on the type of pulse capacitor. The style C series I
have use extended foil construction with a paper or paper-film
dielectric with castor oil as the dielectric fluid. They are rated at
300,000 shots at rated current (100 kA) and voltage. Degradation in
these caps is usually from partial discharges and localized dielectric
damage (particularly at the edges of the foil plates) due to rapid
voltage reversals. This particular style cap is NOT self healing, and it
can indeed short out during the charging cycle. However, the thick steel
case is designed to easily contain a self-faulting cap. They are
designed to "contain" a catastrophic failure without rupturing even when
backfed by three other identical caps connected in parallel. But the
case will definitely be bulged from pressurized gas from the internal
electrical explosion.
Newer high density energy discharge caps use metallized film-foil
construction that is "self healing". This allows the manufacturer to
further push the limits of dielectric stress without risking sudden
failure of the entire capacitor. If a dielectric fault occurs, the short
will blow a small metallized bridge to that section of the capacitor
without causing any other damage. As faults progressively occur and are
cleared, the overall capacitance of the unit steadily decreases. Once
the capacitance has declined by ~5%, the capacitor has reached its end
of life.
BTW, irrespective of whether the cap's case contains the innards, high
energy capacitor failures are always exciting... :^)
Also, a wealth of technical information on high energy capacitor
construction and usage can be found at the General Atomics site:
http://www.gaep.com/technical-bulletins.html
Best wishes,
Bert
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