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Equation 93 · Part 2 · The Bend an Elevator Cannot Fake

Symbol g

ϕ′′=−(g/c2)2/U2=−(ϕ′)2\phi'' = -(g/c^2)^2/U^2 = -(\phi')^2
gg

What this part means

the observer under constant proper acceleration.

Its job in the formula

g is one of the signed contributions combined to compute the quantity on the left.

Where the article explains it

Consider a uniformly accelerated laboratory in otherwise empty, flat spacetime — Einstein’s elevator, given by the exact Rindler metric in coordinates comoving with an observer under constant proper acceleration g : ds2s^2 = -U(Z)^2\,dx02x_0^2 + dZ2Z^2 + dx2x^2 + dy2y^2, \qquad x0x_0 := ct, \qquad U(Z) := 1 + gZc2\frac{gZ}{c^2}.

The passage around this formula

Check it against the elevator directly: ϕ\phi = ln⁡(1+gZ/c2)\ln(1+gZ/c^2) gives ϕ\phi' = (g/c2c^2)/U and ϕ\phi'' = -(g/c2c^2)^2/U2U^2 = -(ϕ\phi')^2 exactly, for every Z , not merely at leading order. The bracket ϕ,ij\phi_{,ij}+ϕ,i\phi_{,i}ϕ,j\phi_{,j} vanishes identically, and so does RiR^i{}_{0j0} — confirming, by direct calculation rather than appeal to intuition, that a uniformly accelerated frame carries exactly zero curvature no matter how large its slope g becomes. The naive second difference of ln⁡\ln U alone, without the quadratic correction, does not vanish in this case — a fact worth stating plainly, because it is exactly the trap a network audit could fall into if it used ϕ,ij\phi_{,ij} by itself as its curvature signal.

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Sources cited in the article section

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