By C. Guy Suits
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Extra resources for Electrical Discharge. With Contributions in Memoriam Including a Complete Bibliography of His Works
These are the values of ip which are plotted in the upper curve of Fig. 1. 8 volts in Table I) the potential must be the same as that of the glass walls, and therefore the sheath on the collector has the same thickness x as that on the walls x0. ) therefore gives the positive ion current corrected for edge effects. 61 cm2) gives the positive ion current density. 71 ma. cm -2 . 00233 j / 7 With a collector surrounded by ionized gas (p = 2) the procedure for cal culating Ip is essentially similar, since equation (53) applies also to this case.
By superimposing an alternating component on the direct current fed to the anode, or by heating the cathode by alternating current, the streamers or individual globules move in sinusoidal paths which reproduce accurately the wave shape of the current even at frequencies up to 1000 cycles. Sometimes the arc-discharge itself oscillates at frequencies in the neighborhood of 1000 cycles and the globules then increase and decrease periodically in brilliancy so that the streamer due to a single globule appears beaded.
13 for 225 volt electrons. 7 volts in agreement with data of Eldridge (Phys. Rev. 20, 456 (1922)). 4 volts). About 36 per cent of the col lisions of 100 volt electrons with mercury atoms yield Class III electrons and the angular deflections are about the same as with argon. Class IV. Secondary Electrons of Moderate Velocity. — These electrons move nearly in random directions and have velocities distributed according to Max well's law corresponding to a temperature T 4 . The current density I 4 (through any imaginary plane from one side to the other) serves as a measure of the num ber of such electrons.
Electrical Discharge. With Contributions in Memoriam Including a Complete Bibliography of His Works by C. Guy Suits