Hinton - The Fourth Dimension.pdf
Hinton - The Fourth Dimension.pdf Hinton - The Fourth Dimension.pdf
66 THE FOURTH DIMENSION In this case all that we see of the plane about which the turning takes place is the line AB. But it is obvious that the axis plane may lie in our space. A point near the plane determines with it a threedimensional space. When it begins to rotate around the plane it does not move anywhere in this three-dimensional space, but moves out of it. A point can no more rotate round a plane in three-dimensional space than a point can move round a line in two-dimensional space. We will now apply the second of the modes of representation to this case of turning about a plane, building up our analogy step by step from the turning in a plane about a point and that in space about a line, and so on. In order to reduce our considerations to those of the greatest simplicity possible, let us realise how the plane being would think of the motion by which a square is turned round a line. Let fig. 34, ABCD be a square on his plane, and represent the two dimensions of his space by the axes Ax, Ay. Now the motion in which the square is turned over about the line AC involves the third dimension. He cannot represent the motion of the whole square in its turning, but he can represent the motions of parts of it. Let the third axis perpendicular to the plane of the paper be called the axis of z. Of the three axes, x, y, z, the plane being can represent any two in his space. Let him then drawn, in fig. 35, two axes, x and z. Here he has in his plane a representation of what exists in the plane which goes off perpendicularly to his space. In this representation the square would not be shown, for in the plane of xy simple the line AB of the square is contained. The plane being then would have before him, in fig. 35, the representation of one line AB of his square and two axes, x and z, at right angles. Now it would be obvious
THE HIGHER WORLD 67 to him that, by a turning such as he knows, by a rotation about a point, the line AB can turn round A, and occupying all the intermediate positions, such as AB1, come, after half a revolution to lie as Ax produced through A. Again, just as he can represent the vertical plane through AB, so he can represent the vertical plane through A’B’, fig. 34, and in a like manner can see that the line A’B’ can turn about the point A’ till it lies in the opposite direction from that which it runs at first. Now these two turnings are not inconsistent. In his plane, if AB is turned about A, and A’B’ about A’, the consiststency of the square would be destroyed, it would be an impossible motion for a rigid body to perform. But in the turning which he studies portion by portion there is nothing inconsistent. Each line in the square can turn in this way, hence he would realise the turning of the whole square as the sum of a number of turnings of isolated parts. Such turnings, if they took place in his plane, would be inconsistent, but by virtue of a third dimension they are consistent, and the result of them all is that the square turns about the line AC and lies in a position in which it is the mirror image of what it was in its first position. Thus he can realise a turning about a line by relinquishing one of his axes, and representing his body part by part. Let us apply this method to the turning of a cube so as to become the mirror image of itself. In our space we can construct three independent axis, x, y, z, shown in fig. 36. Suppose that there is a fourth axis, w, at right angles to each and every one of them. We cannot, keeping all three axes, x, y, z, represent w in our space; but if we relinquish one of our three axes we can let the fourth axis take its place, and we can represent what lies in the square, determined by the two axes we retain and the fourth axis.
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THE HIGHER WORLD 67<br />
to him that, by a turning such as he knows, by a rotation<br />
about a point, the line AB can turn round A, and occupying<br />
all the intermediate positions, such as AB1, come,<br />
after half a revolution to lie as Ax produced through A.<br />
Again, just as he can represent the vertical plane<br />
through AB, so he can represent the vertical plane<br />
through A’B’, fig. 34, and in a like manner can see that<br />
the line A’B’ can turn about the point A’ till it lies in the<br />
opposite direction from that which it runs at first.<br />
Now these two turnings are not inconsistent. In his<br />
plane, if AB is turned about A, and A’B’ about A’, the consiststency<br />
of the square would be destroyed, it would be an<br />
impossible motion for a rigid body to perform. But in<br />
the turning which he studies portion by portion there<br />
is nothing inconsistent. Each line in the square can turn<br />
in this way, hence he would realise the turning of the<br />
whole square as the sum of a number of turnings of<br />
isolated parts. Such turnings, if they took place in his<br />
plane, would be inconsistent, but by virtue of a third<br />
dimension they are consistent, and the result of them all<br />
is that the square turns about the line AC and lies in a<br />
position in which it is the mirror image of what it was in<br />
its first position. Thus he can realise a turning about a<br />
line by relinquishing one of his axes, and representing his<br />
body part by part.<br />
Let us apply this method to the turning of a cube so as<br />
to become the mirror image of itself. In our space we can<br />
construct three independent axis, x, y, z, shown in fig. 36.<br />
Suppose that there is a fourth axis, w, at right angles to<br />
each and every one of them. We cannot, keeping all<br />
three axes, x, y, z, represent w in our space; but if we<br />
relinquish one of our three axes we can let the fourth axis<br />
take its place, and we can represent what lies in the<br />
square, determined by the two axes we retain and the<br />
fourth axis.