ZirkMan said:
And the paradox of how the surface can accelerate towards me locally without accelerating globally remains.
The paradox is a mental construct of your own making, ZirkMan. It is not a real paradox. It results from you having a Newtonian point of view.
So let's back up a bit and look at the Einstein's elevator car thought experiment. I'll replace his elevator car with a rocket to be a bit more modern. Consider these four scenarios:
- The rocket is at rest on the surface of an isolated planet (no sun, no moon) that is similar to the Earth in terms of mass and size. You feel your normal weight.
- The rocket is quiescent and in orbit about this planet. You feel weightless.
- The rocket is quiescent in deep space. You once again feel weightless.
- The rocket is firing its engines in deep space, yielding a constant acceleration of 1g. You no longer feel weightless. Instead you feel your normal weight.
The rest frame of the rocket defines a frame of reference. Newtonian mechanics and general relativity agree on whether this rocket frame is an inertial frame for scenarios 3 and 4 (gravitation is null in these scenarios) but disagree on scenarios 1 and 2. In Newtonian mechanics, the rocket frame is inertial in scenarios 1 and 3 but not in scenarios 2 and 4. In general relativity, the rocket frame is inertial in scenarios 2 and 3 but not in scenarios 1 and 4.
Whether a frame is inertial in Newtonian mechanics can be determined by looking at the behavior of objects known to be free of any external forces. If all such objects maintain a constant velocity the frame is inertial. This inertial/non-inertial characteristic is global in Newtonian mechanics.
Whether a frame is inertial in general relativity can only be determined by making local experiments. Looking out the windows is cheating. You can only using something akin to an accelerometer or ring laser gyro. The inertial/non-inertial characteristic is local (and approximate) in general relativity.
A frame centered on a falling apple is not inertial in Newtonian mechanics but is locally inertial in general relativity. By insisting that the outward acceleration of the surface of the applies globally you are implicitly applying Newtonian logic to a general relativistic concept. To quote the doctor ("Doc, it hurts when I do this"): "Don't do that then."
From the perspective of the falling apple, the dynamics of a nearby falling apple can be described in simple (i.e., inertial) terms. The dynamics of the point on the Earth toward which the apple is falling is, from the perspective of the apple, accelerating toward the apple. You are interpreting this upward acceleration as an outward acceleration. This, coupled with Newtonian think, is what is getting you in trouble. A point on the Earth opposite the point directly beneath the apple is accelerating toward the apple, not outward. You will need to invoke fictitious forces to describe the motion of a falling apple on the other side of the Earth.
To be pedantically correct, you need to invoke those fictitious forces to describe the dynamics of a nearby falling apple as well. The difference is that the fictitious forces on the nearby falling apple are immeasurably small. This is not the case for the apple on the other side of the world.