The nature of the physical worldEddington, Arthur Stanley, Sir
Philosophy
The nature of the physical world
Eddington, Arthur Stanley, Sir
Physics -- Philosophy; Science -- Philosophy
We approached the problem from the point of view that the actual world
with its ten vanishing coefficients of curvature (or its isotropic
directed curvature) has a specialisation which requires explanation; we
were then comparing it in our minds with a world suggested by the pure
mathematician which has entirely arbitrary curvature. But the fact is
that a world of arbitrary curvature is a sheer impossibility. If not
the directed radius, then some other directed length derivable from the
metric, is bound to be homogeneous and isotropic. In applying the ideas
of the pure mathematician we overlooked the fact that he was imagining
[Pg 145]
a world surveyed from outside with standards foreign to it, whereas we
have to do with a world surveyed from within with standards conformable
to it.
The explanation of the law of gravitation thus lies in the fact that
we are dealing with a world surveyed from within. From this broader
standpoint the foregoing argument can be generalised so that it applies
not only to a survey with metre rods but to a survey by optical
methods, which in practice are generally substituted as equivalent.
When we recollect that surveying apparatus can have no extension in
itself but only in relation to the world, so that a survey of space is
virtually a self-comparison of space, it is perhaps surprising that
such a self-comparison should be able to show up any heterogeneity at
all. It can in fact be proved that the metric of a two-dimensional or
a three-dimensional world surveyed from within is necessarily uniform.
With four or more dimensions heterogeneity becomes possible, but it
is a heterogeneity limited by a law which imposes some measure of
homogeneity.
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