“On the _Induction_ of Electric Currents.”... The general
term _induction_ which, as it has been received into
scientific language, may also, with propriety, be used to
express the power which electrical currents may possess of
inducing any particular state upon matter in their immediate
neighbourhood.... I propose to call this action of the current
from the voltaic battery _volta-electric induction_ ... but as
a distinction in language is still necessary, I propose to call
the agency thus exerted by ordinary magnets _magneto-electric
or magne-electric_ induction.
[29] “Experimental Researches,” i. 25, art. 85. This copper disc is
still preserved at the Royal Institution. It was shown in action by the
author of this work, at a lecture at the Royal Institution delivered
April 11th, 1891. Fig. 6 is reproduced in facsimile from Faraday’s
laboratory note-book.
[30] “Experimental Researches,” i. art. 135.
[31] _Ib._, art. 155.
[32] _Ib._, art. 158.
[33] _Ib._, art. 219.
[34] “Experimental Researches,” i. art. 220.
[35] _Ib._, art. 222.
[36] _Ib._, iii. art. 3192.
[37] “Ann. Chim. Phys.,” li. 76, 1832.
[38] The great magnet of the Royal Society, which was at this time lent
to Mr. Christie.
[39] [Original footnote by Faraday.] By magnetic curves, I mean the
lines of magnetic force, however modified by the juxtaposition of
poles, which would be depicted by iron filings; or those to which a
very small magnetic needle would form a tangent.
[40] The entire uselessness as well as the misleading effects of
such unscientific nomenclature might well be taken to heart by those
electrophysiologists and electrotherapeutists who still indulge in the
jargon of “franklinisation,” “faradisation,” and “galvanisation.”
[41] In modern language this would be called the time-integral of
the discharge. The statement is strictly true if the galvanometer
(as was the case with Faraday’s) is one of relatively long period of
oscillation.
[42] From ἄνω _upwards_ and ὁδός _a way_; and κατά _downwards_ and ὁδός
_a way_. The words _cathode_ and _cation_ are now more usually spelled
_kathode_ and _kation_. Faraday sometimes spelled the word _cathion_
(Exp. Res. Art. 1351), as did also Whewell (Hist. of Ind. Sciences,
vol. iii. p. 166).
[43] Literally, _the travellers_, the things which are going.
[44] The term _induction_ appears to have been originally used, in
contradistinction to _contact_ or _conduction_, to connote those
effects which apparently are in the class of actions at a distance.
Thus we may have induction of a charge by a charge, or of a magnet-pole
by a magnet-pole. To these Faraday had added the induction of a current
by a current, and the induction of a current by a moving magnet. Amid
such varying adaptations of the word _induction_, there is much gain
in allotting to the electrostatic induction of charges by charges the
distinguishing name of _influence_, as suggested by Priestley.
Public-domain text, read in full here on John Shaqi.
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