Someone argues: "A freely falling lift removes gravity completely inside it

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · The equivalence principle and gravity as geometry · The equivalence principle and gravity as geometry

The Geometry of Gravity, Ch Accelerated observers, Rindler coordinates and the equivalence principle

Problem

Someone argues: "A freely falling lift removes gravity completely inside it, by the equivalence principle. There is nothing in the statement of the principle that mentions a size, so a freely falling elevator the size of a continent, say ℓ=1000 km\ell = 1000\ \mathrm{km} tall, removes gravity just as completely as a small one. And since the exact metric of a real planet never makes any component vanish above the surface, unlike the Rindler g00g_{00}, there is no coordinate 'edge' of the kind seen in the rocket, so nothing at all limits how large the free-falling region can be." ((a)) Using Earth's radius R⊕=6371 kmR_\oplus = 6371\ \mathrm{km} and the formula for the fractional discrepancy between the exact potential difference and the uniform-field (equivalence-principle) approximation over a height ℓ\ell, namely ℓ/R⊕\ell/R_\oplus, evaluate this fraction for ℓ=1000 km\ell = 1000\ \mathrm{km} and comment on whether it is small. ((b)) Explain why the absence of a vanishing metric component in the exact planetary case does not by itself show that the equivalence principle holds without limit, contrasting a vanishing component with a quantity every observer agrees on. ((c)) State, in one sentence each, what the weak and the Einstein forms of the equivalence principle actually license, and which one is being over-extended by the claim.

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