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Hinton - The Fourth Dimension.pdf

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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

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