Equation 103 · The Bend an Elevator Cannot Fake
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a symmetric rank-two tensor in the local spatial frame of the static observers, with units of inverse time squared — the Eötvös units already standard in gravity-gradient surveying, where 1\, = 10^{-9}\, . Under a rotation of the local spatial axes it transforms as an ordinary rank-two tensor; under a change of which node is used as the additive reference for it is unchanged, because it depends only on derivatives of , never its value; and up to the factor 1 negligible at the one-part-in- 10^9 level for any terrestrial network, it is times the frame component {}_{0j0} of the Riemann tensor in the static observers’ own rest frame — a…
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a symmetric rank-two tensor in the local spatial frame of the static observers, with units of inverse time squared — the Eötvös units already standard in gravity-gradient surveying, where 1\, = 10^{-9}\, . Under a rotation of the local spatial axes it transforms as an ordinary rank-two tensor; under a change of which node is used as the additive reference for it is unchanged, because it depends only on derivatives of , never its value; and up to the factor 1 negligible at the one-part-in- 10^9 level for any terrestrial network, it is times the frame component {}_{0j0} of the Riemann tensor in the static observers’ own rest frame — a genuine curvature quantity, reported honestly as one stated-frame component rather than a coordinate-free scalar invariant, exactly the caveat this construction owes a reader.
Sources cited in the article section
- [11] Apparent Weight of Photons ↗
- [12] Test of Relativistic Gravitation with a Space-Borne Hydrogen Maser ↗
- [8] Atomic Clock Performance Enabling Geodesy Below the Centimetre Level ↗
These citations give research context. Read each source to check which claims it supports.