I have not followed this thread much. I get the impression there is a lot 
of confusion. 

The equivalence principle states there is no distinguishing difference 
between a frame far away in flat spacetime and one in a region of spacetime 
that is curved so long as the frame is small in extent. In other words, it 
there is a curvature R and the dimensions of the frame are d then d << √R. 
This will mean that any test masses in this small frame will be on 
co-parallel geodesics and the local physics is no different than if you are 
on a frame in very distant flat spacetime. The converse of this then is 
that being on an accelerated frame is indistiguishable from being held 
fixed in a gravitational field. The surface of the Earth does that for us. 
Then comparing gravity with acceleration this way the implication is that 
inertial mass is equal to gravitational mass. The previous case indicates a 
way forwards to general relativity with local frames or patches that are 
meshed together in a coordinate atlas and transition function that define 
connection coefficients and curvature.

Is there a better way to do this, Yes! this is what I have been working on. 
Instead of a single small inertial frame consider two frames and in each 
there is one of each EPR pair, The easy part is to show that the 
entanglement is constant so long as the two frames are on geodesic motion. 
This is a sort of extended EP which is potentially useful for quantum 
gravitation. This is in particular if spacetime is built up from quantum 
entangled states. Things becomes much more difficult when black hole 
horizons enter the picture. 

The standard EP is not that hard to understand, and in weak gravitation the 
obvious example of this are weightless objects and astronauts in spacecraft 
and the ISS. In effect this is moving horizontally fast enough to keep 
missing the Earth and it just keeps falling. This is a visual example of 
the EP.

LC

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