I think this thread has managed to answer the original question, which I paraphrase
does General Relativity state that it’s impossible to distinguish an isolated room subjected to constant acceleration from one subject to gravitational acceleration?
After trying both possible answers – yes and no – I believe we’ve shown the answer is
no, for any room with non-zero height, it’s possible to distinguish forces due to gravity from forces due to the room’s acceleration.
There are many ways to state this, some involving the terms “equivalence principle” “infinitesimal” and “tidal force”, but all describe, I think, the same underlying principle.
Simple as this is, I’ve long had a problem applying it. In particular, describing what an un-accelerated observer would observe an accurate clock on a body under acceleration to read relative to his own accurate clock, where both have small masses, and are far from large-mass bodies.
Consider two spaceships far from any star or planet. Initially, A has a velocity of 1000 m/s nearly directly toward B. The distance between A and B is 5000 m. A has an acceleration of 100 m/s/s (a bit over 10 gs). After 10 seconds, A and B are near one another, with relative velocity 0.
Around that instant, what rate relative to his accurate clock would an observer on B observe of an accurate clock on A?
The formula for gravitational time dilation in an accelerated box,

, appears at many reference websites, including
this wikipedia page.

is acceleration, but

is “is the ‘vertical’ distance between the observers”, which I’m unable to understand.
Does anyone know how to calculate the answer to the question above?
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