(365.) Magnetism is remarkable in another important point of view. It
offers a prominent, or “_glaring instance_” of that quality in nature
which is termed _polarity_ (267.), and that under circumstances which
peculiarly adapt it for the study of this quality. It does not appear
that the ancients had any knowledge of this property of the magnet,
though its attraction of iron was well known to them. The first mention
of it in modern times cannot be traced earlier than 1180, though it
was probably known to the Chinese before that time. The polarity of
the magnet consists in this, that if suspended freely, one part of it
will invariably direct itself towards a certain point in the horizon,
the other towards the opposite point; and that, if two magnets, so
suspended, be brought near each other, there will take place a mutual
action, in consequence of which, the positions of both will be
disturbed, in the same manner as would happen if the corresponding
parts of each repelled, and those oppositely directed attracted, each
other; and by properly varying the experiment, it is found that they
really do so. If a small magnet, freely suspended, be brought into
the neighbourhood of a larger one, it will take a position depending
on the position of the _poles_ of the larger one, with respect to its
point of suspension. And it has been ascertained that these and all
other phenomena exhibited by magnets in their mutual attractions and
repulsions are explicable on the supposition of two forces or virtues
lodged in the particles of the magnets, the one predominating at one
end, the other at the other; and such that each particle shall attract
those in which the _opposite_ virtue to its own prevails, and repel
those in which a _similar_ one resides with a force proportional to the
inverse square of their mutual distance.
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