
Schematic: img81.imageshack.us T300-52 iron powder toroid, wound with 50 turns #24 AWG closely together on the primary, and 600 turns of #30 AWG on secondary. Input is a 4.1 kHz square wave from an IRF740 MOSFET connected to ~12 Volt power supply, 50% duty cycle. It's a pulsed DC entering the primary. Since the square wave is DC during the mark phase, and DC goes easily through an inductor, there was quite a bit of current being sucked through even though no load was on the secondary. Nevertheless, as you can see, even with a 1:12 stepup ratio (as would be the case with a sinusoidal input), the square wave resulted in what looks like 3-5 kV from the secondary. With a real load (like a water cell) this would drastically drop, but interesting to see 12 volts turn into a several kilovolts with a mere 600 turns on an iron powder toroid. It's a flyback effect, but I'm not sure how this hand-wound toroid stacks up against a commercial flyback transformer. Once you have a higher voltage signal, then you'd probably need an impedance matching or bridging network between it and the water cell, or perhaps a pulse-forming network to sharpen the spikes and crack the water that way...
stanley
meyer
toroidal
transformer
arc
spark
flyback
high
voltage
hdemartin