The rôle of the space‐charge in atmospheric electricity
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The idea of an electrified atmosphere was generally accepted in Franklin's time, but the experiments of Ermann and Peltier led to the idea of a negatively charged Earth. Lord Kelvin,1 however, saw that both ideas were correct and pointed out that the electric field of the Earth is similar to that of a condenser. This analogy is not very close since only the negative plate is a conducting surface, while the positive plate is the first 8 or 10 kilometers of the atmosphere. The dielectric, moreover, which corresponds with the positive plate, is an ionized gas and for the potentials involved the “leaks” are very significant.
[1] E. Bowie. THE SUMMER NIGHTTIME CLOUDS OF THE SANTA CLARA VALLEY, CALIF. , 1933 .
[2] Joseph G. Brown. The relation of space‐charge and potential gradient to the diurnal system of convection in the lower atmosphere , 1930 .
[3] W. Swann. The atmospheric potential gradient, and a theory as to the cause of its connection with other phenomena in atmospheric electricity, together with certain conclusions as to the expression for the electric force between two parallel charged plates , 1913 .