The form, then, of any portion of matter, whether it be living or dead,
and the changes of form that are apparent in its movements and in its
growth, may in all cases alike be described as due to the action of
force. In short, the form of an object is a “diagram of forces,” in
this sense, at least, that from it we can judge of or deduce the forces
that are acting or have acted upon it: in this strict and particular
sense, it is a diagram,—in the case of a solid, of the forces that
_have_ been impressed upon it when its conformation was produced,
together with those that enable it to retain its conformation; in the
case of a liquid (or of a gas) of the forces that are for the moment
acting on it to restrain or balance its own inherent mobility. In an
organism, great or small, it is not merely the nature of the _motions_
of the living substance that we must interpret in terms of force
(according to kinetics), but also {12} the _conformation_ of the
organism itself, whose permanence or equilibrium is explained by the
interaction or balance of forces, as described in statics.
If we look at the living cell of an Amoeba or a Spirogyra, we see
a something which exhibits certain active movements, and a certain
fluctuating, or more or less lasting, form; and its form at a given
moment, just like its motions, is to be investigated by the help of
physical methods, and explained by the invocation of the mathematical
conception of force.
Now the state, including the shape or form, of a portion of matter,
is the resultant of a number of forces, which represent or symbolise
the manifestations of various kinds of energy; and it is obvious,
accordingly, that a great part of physical science must be understood
or taken for granted as the necessary preliminary to the discussion
on which we are engaged. But we may at least try to indicate, very
briefly, the nature of the principal forces and the principal
properties of matter with which our subject obliges us to deal. Let
us imagine, for instance, the case of a so-called “simple” organism,
such as _Amoeba_; and if our short list of its physical properties and
conditions be helpful to our further discussion, we need not consider
how far it be complete or adequate from the wider physical point of
view[23].
Public-domain text, read in full here on John Shaqi.
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