All this discussion of concrete cases leads up to our consideration
of the modes of acting in the higher organisms. On the strictly
mechanistic manner of thinking the actions of the organism in general
are based on reactions of the tactic kind--inevitable reactions the
nature of which is determined, and which follow a stimulus with a
certainty often fatal to the organism displaying them. Accepting these
tactic reactions as, in general, truly descriptive of the behaviour
of the organism, we can build up a theory of instincts. In their
simplest form instincts are reflexes--tactic movements. In their more
complex forms they are concatenated reflexes, or tactes. A complicated
instinctive action is one consisting of many individual actions, each
of which is the stimulus for the next one; or, of course, it may
also be complex in the sense that several simple reactions proceed
simultaneously, upon simultaneous stimulation of different receptors.
Now the extension of all this to movements of a “higher” grade is
obvious.
Let us note in the first place, that the stimuli so far considered
in all the examples quoted are simple elemental ones. There are, of
course, relatively few such stimuli: gravity, conducted heat (the
kinetic energy of material bodies), radiated heat (the energy of the
ether), electric energy, chemical energy, and mechanical contact or
pressure (including atmospheric vibrations). In all these cases we
have a definite, measurable, physical quantity, with which we must
relate a definite response in the form of a definite measurable,
physico-chemical reaction. There should be a functionality between the
stimulus and response, a definite, quantitative energy-transformation.
To take a concrete example, a certain quantity of light energy falling
upon the receptor organs of Loeb’s caterpillar ought to transform
into another quantity of “nervous energy,” and this travelling in
an analogous way to a “wave of explosion” ought to transform into
an energy quantity of some kind, which initiates another “wave of
explosion” in the muscle substance. All these transformations must
be quantitative ones, and the energy of the individual light must
be traced from the receptor organ to the points in the muscle where
it disturbs a condition of false equilibrium in the substance of
the latter. Nothing less than this is required to demonstrate the
purely physical nature of a reaction, on the part of the organism,
to an external stimulus. It may safely be said that physiological
investigation has not yielded anything even approximating to such an
experimental demonstration.
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