Newtonian Gravity In Curved Space
There are several puzzling things about Newtonian gravity in a
closed universe, not limited to the perennial question about
whether Gauss's law applies in such a context. On a very basic
level, any force-at-a-distance theory gets into trouble if
"distance" is not unique. Any spatial geometry that allows local
curvature will lead to local ambiguities. Even global curvature
seems to imply that the laws would not really be inverse-square.
For example, consider two objects in a spherical universe of
circumference C. If the onjects are separated by a distance r
then they are also separated by a distance C-r in the opposite
direction, so naively applying the inverse square formulation
would give
1 1
F ~ ----- - -------
r^2 (C-r)^2
I remember once computing the value of C that would give the correct
precession of Mercury's orbit. As I recall, it worked out to only
about 7 times the radius of Pluto's orbit, which would make for a
pretty cramped universe. Of course, the above formula isn't really
complete, because the objects are also separated by the distances
r+C, r+2C, r+3C,... and also r-C, r-2C, r-3C,...so the actual inverse
square force law would be in infinite series.
Even more puzzling is an inverse-square force law in a space with
a cylindrical dimension. Consider two points on a cylinder of
circumference C. If the two points are at the same angular position
but separated by an axial distance of R, then the points are obviously
separated by a geodesic of length R. However, they are also separated
by a geodesic of length sqrt(R^2 + C^2) that loops once around the
cylinder. In fact, they are separated by infinitely many geodesics
of length sqrt(R^2 + nC^2), n=0,1,2,..., where n denotes the number
of loops around the cylindrical dimension. This again gives an infinite
series for the complete force law, but now the circumference C need
not be large. You can imagine Kaluza-Klein type universes with curled
up dimensions that would lead to very strange force laws. I suppose
you could try to find a "first-order" law that would yield an infinite
series whose sum approaches an inverse-sqaure law.
Anyway, I think this all goes to show that once you depart from perfect
Euclidean space (and absolute time), it's hard to make much sense out
of action-at-a-distance force laws. This is especially true when the
plane of simultaniety is not unique, since that requires you to look
for action-at-a-distance laws that remain satisfied for any possible
choice of reference frame. I imagine this severely constrains the
possibilities, although I recall reading once about an action-at-a-
distance theory that was consistent with Minkowski space-time (locally).
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