Essays: Scientific, Political, & Speculative; Vol. 2 of 3: Library Edition (1891), Containing Seven Essays not before Republished, and Various other Additions.Spencer, Herbert
Philosophy
Essays: Scientific, Political, & Speculative; Vol. 2 of 3: Library Edition (1891), Containing Seven Essays not before Republished, and Various other Additions.
Spencer, Herbert
Philosophy; Political science; Science
On one point an addition seems needful to exclude a misconstruction
apt to arise. The description of the mutually-produced molecular
perturbations, opposite in their kinds, as resulting in waves that are
propagated away from the place of disturbance, and that cancel when
brought into relation, is met by the criticism that waves, proceeding
in opposite directions and meeting, do not mutually cancel, but,
passing one another, proceed onwards. There are, however, two respects
in which the parallelism does not hold, between the waves referred
to and the waves I have described, which perhaps cannot rightly be
called waves. The waves referred to, as those on the surface of a
liquid, {185} are such that each consists of two opposite deviations
from a mean state. Each shows excess and defect. A series of them is
a series of _plus_ and _minus_ divergences; and if two such series
meet one another, they do not cancel. But there is no analogy between
this case and a case in which the whole effect propagated in one
direction is a _plus_ motion, and the whole effect propagated in the
opposite direction is a _minus_ motion—that is, _plus_ and _minus_
changes in other motions. These, if equal in amount, will cancel when
they meet. If one is a continual addition to motion in a certain
direction, and the other a corresponding subtraction from motion in
that direction, the two, when added together, must produce zero. From
another point of view the absence of parallelism between the two
cases may be equally well seen. Waves of the kinds instanced as not
cancelling one another, are waves produced by some force foreign to
the medium exhibiting them—an extrinsic force. Hence, proceeding from
the place of initiation, they are necessarily, considered in their
totalities, _positive_ in whatever directions they travel; and hence,
too, when conducted round so as to meet, an exaggerated perturbation
will result. But in the simplest of the cases here dealt with (that
of contact-electricity) the perturbation is not of extrinsic origin,
but of intrinsic origin. There is no external activity at the expense
of which the quantity of motion in the disturbed matter is positively
increased. The activity, being such only as is internally possessed,
can generate no more motion than already exists; and therefore whatever
gain of motion arises anywhere in the molecules must be at the cost of
an equal loss elsewhere. Here perturbation cannot be a _plus_ motion
in all directions from the place of initiation; but any _plus_ motion
continually generated can result only from an equal and opposite
_minus_ motion continually generated; and the mutual cancelling becomes
a corollary from the mutual genesis.
In the course of the discussions which I have had, the {186} following
way of presenting the argument has occurred to me.
Public-domain text, read in full here on John Shaqi.
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