The Principles of Biology, Volume 2 (of 2)Spencer, Herbert
Science
The Principles of Biology, Volume 2 (of 2)
Spencer, Herbert
Biology
That the property specially displayed by nerve, is a property which
protoplasm possesses in a lower degree, is manifest. The sarcode
of a Rhizopod and the substance of an unimpregnated ovum, exhibit
movements that imply a propagation of stimulus from one part of
the mass to another. We have not far to seek for a probable origin
of this phenomenon. There is good reason for ascribing it to the
extreme instability of the organic colloids of which protoplasm
consists. These, in common with colloids in general, assume
different isomeric forms with great facility; and they display not
simply isomerism but polymerism. Further, this readiness to undergo
molecular re-arrangement, habitually shows itself in colloids by
the rapid propagation of the re-arrangement from part to part. As
Prof. Graham has shown, matter in this state often “pectizes” almost
instantaneously--a touch will transform an entire mass. That is to say,
the change of molecular state once set up at one end, spreads to the
other end--there is a progress of a stimulus to change; and this is
what we see in a nerve. So much being understood, let us re-state the
case more completely.
Molecular change, implying as it does motion of molecules, communicates
motion to adjacent molecules; be they of the same kind or of a
different kind. If the adjacent molecules, either of the same kind or
of a different kind, be stable in composition, a temporary increase
of oscillation in them as wholes, or in their parts, may be the only
result; but if they are unstable there are apt to arise changes of
arrangement among them, or among their parts, of more or less permanent
kinds. Especially is this so with the complex molecules which form
colloidal matter, and with the organic colloids above all. Hence it is
to be inferred that a molecular disturbance in any part of a living
animal, set up by either an external or internal agency, will almost
certainly disturb and change some of the surrounding colloids not
originally implicated--will diffuse a wave of change towards other
parts of the organism: a wave which will, in the absence of perfect
homogeneity, travel further in some directions than in others. Let us
ask next what will determine the differences of distance travelled in
different directions. Obviously any molecular agitation spreading from
a centre, will go furthest along routes that offer least resistance.
What routes will these be? Those along which there lie most molecules
that are easily changed by the diffused molecular motion, and which
yet do not take up much molecular motion in assuming their new states.
Molecules which are tolerably stable will not readily propagate the
agitation; for they will absorb it in the increase of their own
oscillations, instead of passing it on. Molecules which are unstable
but which, in assuming isomeric forms, absorb motion, will not readily
propagate it; since it will disappear in working the changes in them.
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