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Hinton - The Fourth Dimension.pdf

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THE HIGHER WORLD 69<br />

simply the plane of xy and the square base of the<br />

w<br />

cube ACEG, fig. 39, is all that could<br />

be seen of it. Let now the w axis<br />

y<br />

take the place of the z axis and<br />

E<br />

G<br />

x<br />

we have, in fig. 39 again, a representation<br />

of the space of xyw, in<br />

A C which all that exists of the cube is<br />

Fig. 39. its square base. Now, by a turning<br />

of x to w, this base can rotate around the line AE, it is<br />

w<br />

shown on its way in fig. 40, and<br />

finally it will, after half a revolution,<br />

y<br />

G<br />

lie on the other side of the y axis. In<br />

a similar way we may rotate<br />

E<br />

C sections parallel to the base of the<br />

A<br />

Fig. 40.<br />

x<br />

xw rotation, and each of them comes<br />

to run in the opposite direction from<br />

that which they occupied at first.<br />

Thus again the cube comes from the position of fig. 36<br />

H F z<br />

to that of fig. 41. In this x to<br />

w turning, we see that it<br />

takes place by the rotations of<br />

D<br />

y<br />

B<br />

sections parallel to the front<br />

G<br />

E<br />

face about lines parallel to AB,<br />

or else we may consider it as<br />

C A x x<br />

nd st<br />

2 position 1 position<br />

Fig. 41.<br />

consisting of the rotations of<br />

sections parallel to the base<br />

about lines parallel to AE. It<br />

is a rotation of the whole cube about the plane ABEF.<br />

Two separate sections could not rotate about two separate<br />

lines in our space without conflicting, but their motion is<br />

consistent when we consider another dimension. Just,<br />

then, as a plane being can think of rotation about a line as<br />

a rotation about a number of points, these rotations not<br />

interfering as they would if they took place in his twodimensional<br />

space, so we can think of a rotation about a

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