those at a distance, and which comprehend the phenomena of the
electric discharge. Having considered, in the preceding paper, the
process by which the former condition is established, and which consists in the successive polarization of series of contiguous particles
of the interposed insulating dielectric; the author here proceeds to
trace the process, which, taking place consequently on simple induction, terminates in that sudden, and often violent interchange of
electric forces constituting disruption, or the electric discharge. He
investigates, by the application of his theory, the gradual steps of
transition which may be traced between perfect insulation on the
one hand, and perfect conduction on the other, derived from the
varied degrees of specific electric relations subsisting among the рarticular substances interposed in the circuit: and from this train of
reasoning he deduces the conclusion that induction and conduction
not only depend essentially on the same principles, but that they
may be regarded as being of the same nature, and as differing merely
in degree.
The fact ascertained by Professor Wheatstone, that electric conduction, even in the most perfect conductors, as the metals, requires for its completion a certain appreciable time, is adduced in corroboration of these views; for any retardation, however small, in the transmission of electric forces can result only from induction; the degree of retardation, and, of course, the time employed, being proportional to the capacity of the particles of the conducting body for retaining a given intensity of inductive charge. The more perfect insulators, as lac, glass and sulphur, are capable of retaining electricity of high intensity; while, on the contrary, the metals and other excellent conductors, possess no power of retention when the intensity of the charge exceeds the lowest degrees. It would appear, however, that gases possess a power of perfect insulation, and that the effects generally referred to their capacity of conduction, are only the results of the carrying power of the charged particles either of the gas, or of minute particles of dust which may be present in them and they perhaps owe their character of perfect insulators to their peculiar physical state, and to the condition of separation under which their particles are placed. The changes produced by heat on the conducting power of different bodies is not uniform; for in some, as sulphuret of silver and fluoride of lead, it is increased; while in others, as in the metals and the gases, it is diminished by an augmentation of temperature.
One peculiar form of electric discharge that which attends electrolyzation, an effect involving previous induction; which induction has been shown to take place throughout linear series of polarized particles, in perfect accordance with the views entertained by the author of the general theory of inductive action. The peculiar feature of this mode of discharge, however, is in its consisting, not in a mere interchange of electric forces at the adjacent poles of contiguous particles, but in their actual separation into their two constituent particles; those of each kind travelling onwards in contrary directions, and retaining the whole amount of the force they had ac-
