bapowell said:
Regarding 2., it might be of interest to point out that some practitioners prefer not to encourage the literal geometric interpretation of the theory. For instance, Weinberg in his seminal text "Gravitation and Cosmology" chooses not elevate geometry to a staring role, but rather emphasizes that the "peculiar empirical properties", like Einstein's equivalence principle, just happen to be expressed in the mathematical language of differentiable manifolds. This has implications for whether we view gravity as a force or merely as a "geometrical effect".
Consider electromagnetism, which is based on U(1) gauge symmetry in the Standard Model. It is perfectly reasonable to cast this theory as one of geometry: we find that the vector potential plays the role of the connection, describing how "vectors" twist and contort as they are parallel transported through the admittedly abstract U(1) internal space. Further, the electromagnetic field strength tensor literally measures the curvature of this internal space. Do these ideas stop us from also considering the vector potential as a gauge field whose quanta are the literal mediators of the electromagnetic force? No: the geometric interpretation of the U(1) theory is not emphasized, favoring instead its particle physics incarnation in terms of gauge bosons.
General relativity is no more "geometric" than the gauge theories of particle physics, the primary difference being that the geometry of general relativity is actual space and time, rather than abstract "internal" group spaces, and so it is emphasized. Emphasis aside, if there really is no fundamental distinction, why do we single out gravity as being a "geometric effect" while the other interactions are particle mediated?
There are many things that make a geometrical interpretation of GR the most natural one, sometimes even the only one!
One thing is that for other interaction, a geometrical interpretation requires the introduction of a new spooky space which is not desirable. But about GR, we have space-time which I directly observable.
Also, when I think about the effects that gravitation can have on space-time, it seems very natural to me to have a geometrical interpretation for GR. So natural that I think its being suggested by nature itself. If we say that gravitation is, like other interactions, a field on Minkowski space-time, then there should be some extra explanation that how it has the observed effects on space and time.
Also all attempts at deriving Einstein's equations using QFT methods, concluded that the field(s) behaved so much like the geometrical properties of space-time that no one bothers to name them differently. And now we have at our disposal a space(space-time) and a theory describing its properties. Not accepting that gravity is the result of the geometry of space-time and looking for another point of view seems a child's nag to me!(No disrespect intended but that's really how it seems to me.)
For one good thing, you can look at section 7.3 of Gravitation by Misner, Thorne and Wheeler.
This is my idea about GR but I should confess that I think its more wrong to prevent a physical idea to grow. So, although I like the idea that gravitation is caused by space-time's geometry and think this is GR's correct interpretation and will oppose other interpretations, But I'll be happy to see such theories to grow and be discussed. Its strange that I have this two sided feeling that I oppose it but don't want it to be absent but that's how I feel.
I should also say that this is my idea about GR in case I believe GR is the correct theory for gravity. I know its the mainstream theory for gravity, so I think its probably the correct one but I like to investigate its alternatives too. So if one day, one of GR's alternatives turns out to be better, I will change to that and so, that day, I won't attach gravity to space-time's geometry.
(oops...did I talk too much?!...sorry!:D)