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3<br />
APPLICATION TO KANT’S THEORY OF EXPERIENCE 113<br />
on to a greater multiplicity of dimensions, and the<br />
significance of the process here briefly explained<br />
becomes more apparent.<br />
Take three mutually rectangular axes in space 1, 2, 3<br />
c<br />
b a<br />
a<br />
b<br />
c<br />
a b c<br />
1 2<br />
Fig. 59.<br />
(fig. 59), and on each mark three points,<br />
the common meeting point being the<br />
first on each axis. <strong>The</strong>n by means of<br />
these three points on each axis, we<br />
define 27 positions, 27 points in a<br />
cubical cluster, shown in fig. 60, the<br />
same method of co-ordination being<br />
used as has been described before.<br />
Each of these positions can be named by means of the<br />
axes and the points combined.<br />
Thus, for instance, the one marked by an asterisk can<br />
3<br />
1 2<br />
Fig. 60.<br />
be called 1c, 2b, 3c, because it is<br />
opposite to c on 1, to b on 2, to<br />
c on 3.<br />
Let us now treat of the states of<br />
consciousness corresponding to these<br />
positions. Each point represents a<br />
composite of posits, and the manifold<br />
of consciousness corresponding<br />
to them is of a certain complexity.<br />
Suppose now the constituents, the points on the axes,<br />
to interchange arbitrarily, any one to become any other,<br />
and also the axes 1, 2 and 3, to interchange amongst<br />
themselves, any one to become any other, and to be subject<br />
to no system or law, that is to say, that order does<br />
not exist, and that the points which run abc on each axis<br />
may run bac, and so on.<br />
<strong>The</strong>n any one of the states of consciousness represented<br />
by the points in the cluster can become any other. We<br />
have a representation of a random consciousness of a<br />
certain degree of complexity.