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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