account.

Now could it be shown that the two-dimensional symmetry observed in
nature is the result of a three-dimensional movement, the right-and
left-handed symmetry of solids would by analogy be the result of a
_four_-dimensional movement. Such revolution (about a plane) would
be easily achieved, natural and characteristic, in four space, just
as the analogous movement (about a line) is easy, natural, and
characteristic, in our space of three dimensions.


OTHER ALLIED PHENOMENA

In the mirror image of a solid we have a representation of what
would result from a four-dimensional revolution, the surface of the
mirror being the plane about which the movement takes place. If such
a change of position were effected in the constituent parts of a
body as a mirror image of it _represents_, the body would have
undergone a revolution in the fourth dimension. Now two varieties of
tartaric acid crystallize in forms bearing the relation to one
another of object to mirror image. It would seem more reasonable to
explain the existence of these two identical, but reversed,
varieties of crystal, by assuming the revolution of a single variety
in the fourth dimension, than by any other method.

There are two forms of sugar found in honey, dextrose and levulose.
They are similar in chemical constitution, but the one is the
reverse of the other when examined by polarized light--that is, they
rotate the plane of polarization of a ray of light in opposite ways.
If their atoms are conceived to have the power of motion in the