Equation 72 · The Bend an Elevator Cannot Fake
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the height. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.
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This is an exact solution describing flat Minkowski spacetime in non-inertial coordinates, not a weak-field approximation. A clock held static at height Z has d = U(Z)\,dt exactly, so two such clocks compare frequencies as / = U()/U() to all orders — the same exact redshift formula an accelerating rocket produces for light climbing or falling inside it. The node potential is = U(Z) = , and its first derivative at Z=0 is ' = g/ : a nonzero, entirely real, measurable slope. A network of clocks bolted to this elevator’s walls would report exactly the nonzero edge data a network in a genuine gravitational field reports at the same order. If…
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This is an exact solution describing flat Minkowski spacetime in non-inertial coordinates, not a weak-field approximation. A clock held static at height Z has d = U(Z)\,dt exactly, so two such clocks compare frequencies as / = U()/U() to all orders — the same exact redshift formula an accelerating rocket produces for light climbing or falling inside it. The node potential is = U(Z) = , and its first derivative at Z=0 is ' = g/ : a nonzero, entirely real, measurable slope. A network of clocks bolted to this elevator’s walls would report exactly the nonzero edge data a network in a genuine gravitational field reports at the same order. If a nonzero slope alone were curvature, this elevator would be curved. It is not; by construction its spacetime is exactly flat, and the geodesic deviation between any two nearby free-falling test particles inside it is exactly zero at every instant, because flatness is a property of the manifold and does not care what coordinates — accelerated, rotating, or otherwise — a particular family of observers happens to use.
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