LAWS OF ELECTROLYTIC CONDUCTION
All these facts combine into, I think, an irresistible mass of evidence, proving the truth of the important proposition which I at first laid down—namely, that the chemical power of a current of electricity is in direct proportion to the absolute quantity of electricity which passes. They prove, too, that this is not merely true of one substance, as water, but generally with all electrolytic bodies; and, further, that the results obtained with any one substance do not merely agree amongst themselves, but also with those obtained from other substances, the whole combining together into one series of definite electrochemical actions. I do not mean to say that no exceptions will appear; perhaps some may arise, especially amongst substances existing only by weak affinity; but I do not expect that any will seriously disturb the result announced. If, in the well considered, well examined, and, I may surely say, well-ascertained doctrines of the definite nature of ordinary chemical affinity, such exceptions occur, as they do in abundance, yet, without being allowed to disturb our minds as to the general conclusion, they ought also to be allowed if they should present themselves at this, the opening of a new view of electrochemical action; not being held up as obstructions to those who may be engaged in rendering that view more and more perfect, but laid aside for a while, in hopes that their perfect and consistent explanation will ultimately appear.
The doctrine of definite electrochemical action just laid down, and, I believe, established, leads to some new views of the relations and classifications of bodies associated with or subject to this action. Some of these I shall proceed to consider. In the first place, compound bodies may be separated into two great classes namely, those which are decomposable by the electric current, and those which are not: of the latter, some are conductors, others non-conductors, of voltaic electricity.[1] The former do not depend for their decomposability upon the nature of their elements only; for, of the same two elements, bodies may be formed, of which one shall belong to one class and another to the other class; but probably on the proportions also. It is further remarkable, that with very
few, if any, exceptions, these decomposable bodies are exactly
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- ↑ I mean here, by voltaic electricity, merely electricity from a most abundant source, but having very small intensity.
