Haelfix said:
Actually I was under the impression that departure from spherical symmetry breaks the geoid surface symmetry, but whatever its a small point, the Earth isn't quite spherical or elliptical, it has a certain equatorial bulge. I haven't done the full calculation so I am not entirely sure about it.
I'm not sure which symmetry you think is broken?
If the Earth were actually a ball of fluid in equilibrium (or a solid core with a fluid-covered surface), all clocks on that fluid surface would run at the same rate.
The Earth does not actually have the shape described above, but I won't get into details of the (small) errors. The actual shape of the Earth is quite close to this "idealized" shape.
The equatorial bulge caused by the Earth's rotation does not "mess up" the constancy of rate of clocks on the Earth surface - it's an intergal part of why clocks on the Earth's surface run at the same rate.
http://www.physicstoday.org/vol-58/iss-9/p12.html
and the previously mentioned
http://relativity.livingreviews.org/open?pubNo=lrr-2003-1&page=node3.html
both discuss this. Note that Einstein himself in his original SR paper, like the OP in this thread, predicted that clocks at the poles would run at a different rate than clocks on the equator. It wasn't until much later when Einstein developed GR that he realized that the clocks would run at the same rate at both locations.
The detailed argument gets rather technical, but the short version is easy to understand. If two observers can exchange light signals without any red or blue shift, they will infer that their clocks run at the same rate.
Because the Earth is an equipotential surface, we can infer that there will be no red or blue shift in transmitted signals.
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Here is a slightly more technical argument that addresses the problem. Consider the rotating fluid-covered Earth as a static problem in GR (static because the metric coefficients do not vary with time).
The force of gravity in the local coordinate system will be a vector, given by \nabla g_{00}.
The fluid has the property that the fluid surface is always perpendicular to the local gravitational field if it is in equilibrium.
Therfore the equilibrium fluid has the property that the fluid surface is at a constant value of g_{00}.