induction as an action at a distance and in straight
lines, long indisposed me to the view I have just
stated; and though I always watched for opportunities
to prove the opposite opinion, and made such experiments
occasionally as seemed to bear directly on the point,
as, for instance, the examination of electrolytes,
solid and fluid, whilst under induction by polarized
light (951. 955.), it is only of late, and by degrees,
that the extreme generality of the subject has urged
me still further to extend my experiments and publish
my view. At present I believe ordinary induction
in all cases to be an action of contiguous particles
consisting in a species of polarity, instead of being
an action of either particles or masses at sensible
distances; and if this be true, the distinction and
establishment of such a truth must be of the greatest
consequence to our further progress in the investigation
of the nature of electric forces. The linked condition
of electrical induction with chemical decomposition;
of voltaic excitement with chemical action; the transfer
of elements in an electrolyte; the original cause
of excitement in all cases; the nature and relation
of conduction and insulation of the direct and lateral
or transverse action constituting electricity and
magnetism; with many other things more or less incomprehensible
at present, would all be affected by it, and perhaps
receive a full explication in their reduction under
one general law.
1166. I searched for an unexceptionable test
of my view, not merely in the accordance of known
facts with it, but in the consequences which would
flow from it if true; especially in those which would
not be consistent with the theory of action at a distance.
Such a consequence seemed to me to present itself
in the direction in which inductive action could be
exerted. If in straight lines only, though not
perhaps decisive, it would be against my view; but
if in curved lines also, that would be a natural result
of the action of contiguous particles, but, as I think,
utterly incompatible with action at a distance, as
assumed by the received theories, which, according
to every fact and analogy we are acquainted with, is
always in straight lines.
1167. Again, if induction be an action of contiguous
particles, and also the first step in the process
of electrolyzation (1164. 919.), there seemed reason
to expect some particular relation of it to the different
kinds of matter through which it would be exerted,
or something equivalent to a specific electric
induction for different bodies, which, if it existed,
would unequivocally prove the dependence of induction
on the particles; and though this, in the theory of
Poisson and others, has never been supposed to be
the case, I was soon led to doubt the received opinion,
and have taken great pains in subjecting this point
to close experimental examination.