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148<br />
THE FOURTH DIMENSION<br />
you first saw. This finished up the cube—it is the further<br />
face in the unknown dimension.<br />
<strong>The</strong> white line, which extends in length just like the<br />
red or the yellow, you do not see as extensive; you apprehend<br />
it simply as an enduring white point. <strong>The</strong> null<br />
point, under the condition of movement of the cube,<br />
vanishes in a moment, the lasting white point is really<br />
your apprehension of a white line, running in the unknown<br />
dimension. In the same way the red line of the face by<br />
which the cube is first in contact with the plane lasts only<br />
a moment, it is succeeded by the pink line, and this pink<br />
line lasts for the inside of a minute. This lasting pink<br />
line is your apprehension of a surface, which extends in<br />
two dimensions just like the orange surface extends, as you<br />
know it, when the cube is at rest.<br />
But the plane creature might answer, “This orange<br />
object is substance, solid substance, bounded completely<br />
and on every side.”<br />
Here, of course, the difficulty comes in. His solid is our<br />
surface—his notion of a solid is our notion of an abstract<br />
surface with no thickness at all.<br />
We should have to explain to him that, from every point<br />
of what he called a solid, a new dimension runs away.<br />
From every point a line can be drawn in a direction<br />
unknown to him, and there is a solidity of a kind greater<br />
than that which he knows. This solidity can only be<br />
realised by him by his supposing an unknown direction,<br />
by motion in which what he conceives to be solid matter<br />
instantly disappears. <strong>The</strong> higher solid, however, which<br />
extends in this dimension as well as in those which he<br />
knows, lasts when a motion of that kind takes place,<br />
different sections of it come consecutively in the plane of<br />
his apprehension, and take the place of the solid which he<br />
at first sign conceives to be all. Thus, the higher solid—our<br />
solid in contradistinction to his area solid, his two-