The discharge was an atmospheric pressure Glow Discharge not an Arc.
" Most of the voltage between anode and cathode is represented by the cathode fall Vc near the cathode. Aston found experimentally that the electric field is greatest at the cathode, and falls linearly to zero at the end of the cathode fall in the negative glow. This linear decrease means that the potential rises parabolically: V(x) = (2Vc/d2)x(x - 2d). This means that there is a constant positive space charge in the region of amount Vc/2pd2, and the field at the cathode is Eo = 2Vc/d. If K is the mobility of the positive ions, then the positive ion current can be found. The electron current is ? times this, so the total current density at the cathode is jo = Vc2K(1 + ?)/pd3"
"Fast ion bombardment causes sputtering of the cathode material. The rate of sputtering is proportional to (Vc - V), where V is the normal cathode fall, and Vc the established cathode fall. 850V would not be an unusual figure, where V = 200V, say. The exact mechanism of sputtering is in doubt, but it seems that cathode material is ejected to the cathode surface, and then evaporated by the local heating. The rate of deposition obeys the inverse-square law. The films produced are quite coherent and uniform. Silver sputters relatively easily, aluminum with difficulty. Where cathode surfaces are specially prepared, perhaps with low-work function substances as in thermionic cathodes, sputtering can destroy them quickly, even at relatively low overvoltages. There seems to be little sputtering at the normal cathode fall. The electrodes of glow lamps are treated with low-work-function materials, so they are injure!
d by overcurrent, and their striking voltages may rise."
----- Original Message -----From: TP SparberSent: 6/17/2006 6:34:12 AMSubject: [Vo]: Re: Pressure Cooker Fractional OrbitsPosted earlier:>> The arc drops the transformer output to 1,000 volts or less at 0.06 amps> so there wasn't enough input energy to account for the pressure rise.>Mizuno's experiments come to mind here, except the discharge is to the waterpool surface is though the air (N2, O2, Ar, CO2, ) and H2O vapor rather than inthe water.Mizuno's early tungsten in water arc experiments (1998) by comparison:The ion energy bombarding the pool surface is set by the cathodefall potential which is probably not more than 150 volts or less.This means that a proton (or some deuterons in the water)can penetrate intoan oxygen, nitrogen, or argon electron cloud setting up Auger Effect "cascades"by proton/deuteron capture of inner shell electrons with an energy releasethat can substantially multiply the energy input.Fred