The nature of the physical worldEddington, Arthur Stanley, Sir
Philosophy
The nature of the physical world
Eddington, Arthur Stanley, Sir
Physics -- Philosophy; Science -- Philosophy
Of the two alternatives—a curved manifold in a Euclidean space of ten
dimensions or a manifold with non-Euclidean geometry and no extra
[Pg 159]
dimensions—which is right? I would rather not attempt a direct answer,
because I fear I should get lost in a fog of metaphysics. But I may
say at once that I do not take the ten dimensions seriously; whereas
I take the non-Euclidean geometry of the world very seriously, and I
do not regard it as a thing which needs explaining away. The view,
which some of us were taught at school, that the truth of Euclid’s
axioms can be seen intuitively, is universally rejected nowadays.
We can no more settle the laws of space by intuition than we can
settle the laws of heredity. If intuition is ruled out, the appeal
must be to experiment—genuine open-minded experiment unfettered by
any preconception as to what the verdict ought to be. We must not
afterwards go back on the experiments because they make out space to
be very slightly non-Euclidean. It is quite true that a way out could
be found. By inventing extra dimensions we can make the non-Euclidean
geometry of the world depend on a Euclidean geometry of ten dimensions;
had the world proved to be Euclidean we could, I believe, have made its
geometry depend on a non-Euclidean geometry of ten dimensions. No one
would treat the latter suggestion seriously, and no reason can be given
for treating the former more seriously.
I do not think that the six extra dimensions have any stalwart
defenders; but we often meet with attempts to reimpose Euclidean
geometry on the world in another way. The proposal, which is made quite
unblushingly, is that since our measured lengths do not obey Euclidean
geometry we must apply corrections to them—cook them—till they do. A
closely related view often advocated is that space is neither Euclidean
nor non-Euclidean; it is all a matter of convention and we are free
to adopt any geometry we choose.[27] Naturally if we hold ourselves
[Pg 160]
free to apply any correction we like to our experimental measures we
can make them obey any law; but was it worth while saying this? The
assertion that any kind of geometry is permissible could only be made
on the assumption that lengths have no fixed value—that the physicist
does not (or ought not to) mean anything in particular when he talks
of length. I am afraid I shall have a difficulty in making my meaning
clear to those who start from the assumption that my words mean nothing
in particular; but for those who will accord them some meaning I will
try to remove any possible doubt. The physicist is accustomed to state
lengths to a great number of significant figures; to ascertain the
significance of these lengths we must notice how they are derived; and
we find that they are derived from a comparison with the extension of
a standard of specified material constitution. (We may pause to notice
that the extension of a standard material configuration may rightly
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