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THE SIMPLEST FOUR-DIMENSIONAL SOLID 161<br />
but the thought of an abstract boundary, the face of<br />
a cube.<br />
Let us now take our eight coloured cubes, which form<br />
a cube in space, and ask what additions we must make<br />
to them to represent the simplest collection of four-dimensional<br />
bodies—namely, a group of them of the same extent<br />
in every direction. In plane space we have four squares.<br />
In solid space we have eight cubes. So we should expect<br />
in four-dimensional space to have sixteen four-dimensional<br />
bodies—bodies which in four-dimensional space<br />
correspond to cubes in three-dimensional space, and these<br />
bodies we call tesseracts.<br />
Given then the null, white, red, yellow cubes, and<br />
those which make up the block, we<br />
notice that we represent perfectly<br />
well the extension in three directions<br />
(fig. 98). From the null point of the<br />
x<br />
(Orange hidden)<br />
Fig. 98.<br />
null cube, travelling one inch, we<br />
come to the white cube; travelling<br />
one inch away we come to the yellow<br />
cube; travelling one inch up we come<br />
to the red cube. Now, if there is a<br />
fourth dimension, then travelling<br />
from the same null point for one<br />
inch in that direction, we must come to the body lying<br />
beyond the null region.<br />
I say null region, not cube; for with the introduction<br />
of the fourth dimension each of our cubes must become<br />
something different from cubes. If they are to have<br />
existence in the fourth dimension, they must be “filled<br />
up from” in this fourth dimension.<br />
Now we will assume that as we get a transference from<br />
null to white going in one way, from null to yellow going<br />
in another, so going from null in the fourth direction we<br />
have a transference from null to blue, using thus the