Abstract
It has long been known that above onset of steady positive wire corona with coaxial cylindrical geometry, Townsend's relation of 1914 relating current i and over-voltage, VVg, of the form VVg=BiV applies over a considerable range. This law is deduced assuming a constant potential across a zone of limited constant ionizing radius. Such assumption implies a constant Townsend amplification factor for ionization by collision, a fact just recently experimentally established by Colli, Facchini, and Gatti. The corona current i on this theory, however, increases many times despite constant amplification factor. It is shown that this occurs by slight temporary raising of the amplification factor producing a rapid proliferation of ionizing sequences over the anode surface, increasing current and space charge density, but maintaining essentially constant amplification factor. This action has a bearing on the spread of the normal glow discharge over the cathode.