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Hinton - The Fourth Dimension.pdf

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70<br />

THE FOURTH DIMENSION<br />

plane as the rotation of a number of sections of a body<br />

about a number of lines in a plane, these rotations not<br />

being inconsistent in a four-dimensional space as they are<br />

in three-dimensional space.<br />

We are not limited to any particular direction for the<br />

lines in the plane about which we suppose the rotation<br />

of the particular sections to take place. Let us draw<br />

the section of the cube, fig. 36, through A, F, C, B, forming<br />

a sloping plane. Now since the fourth dimension is at<br />

right angles to every line in our space it is at right<br />

angles to this section also. We can represent our space<br />

by drawing an axis at right angles to the plane ACEG, our<br />

space is then determined by the plane ACEG, and the perpendicular<br />

axis. If we let this axis drop and suppose the<br />

fourth axis, w, to take its place, we have a representation of<br />

the space which runs off in the fourth dimension from the<br />

plane ACEG. In this space we shall see simply the section<br />

ACEG of the cube, and nothing else, for one cube does not<br />

extend to any distance in the fourth dimension.<br />

If, keeping this plane, we bring in the fourth dimension,<br />

we shall have a space in which simply this section of<br />

the cube exists and nothing else. This section can turn<br />

about the line AF, and parallel sections can turn about<br />

z<br />

parallel lines. Thus in considering<br />

the rotation about<br />

a plane we can draw any<br />

D F lines we like and consider<br />

the rotation as taking place<br />

G H<br />

x in sections about them.<br />

To bring out this point<br />

C E<br />

more clearly, let us take two<br />

y<br />

parallel lines, A and B, in<br />

A B<br />

the space of xyz, and let CD<br />

Fig. 42.<br />

and EF be two rods running<br />

above and below the plane of xy, from these lines. If we

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