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Hinton - The Fourth Dimension.pdf

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SECOND CHAPTER IN THE HISTORY OF FOUR SPACE 51<br />

A shear does not alter the volume of a body: thus an<br />

inhabitant living in such a world would look on a body<br />

sheared as we look on a body rotated. He would say<br />

that it was the same shape, but had turned a bit<br />

round.<br />

Let us imagine a Pythagoras in this world going to<br />

work to investigate, as is his wont.<br />

Fig. 27. Fig. 28.<br />

Fig. 27 represents a square unsheared. Fig. 28<br />

represents a square sheared. It is not the figure into<br />

which the square in fig. 27 would turn, but the result of<br />

shear on some square not drawn. It is a simple slanting<br />

placed figure, taken now as we took a simple slanting<br />

placed square before. Now, since bodies in this world of<br />

shear offer no internal resistance to shearing, and keep<br />

their volume when sheared, an inhabitant accustomed to<br />

them would not consider that they altered their shape<br />

under shear. He would call ACDE as much as square as<br />

the square in fig. 27. We will call such figures shear<br />

squares. Counting the dots in ACDE, we find—<br />

A<br />

2 inside = 2<br />

4 at corners = 1<br />

or a total of 3.<br />

Now, the square on the side AB has 4 points, that on BC<br />

has 1 point. Here the shear square on the hypothenuse<br />

has not 5 points by 3; it is not the sum of the squares on<br />

the side, but the difference.<br />

E<br />

C<br />

B<br />

D

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