A Mössbauer source is mounted at the top of a cathedral spire of height m and the…

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

Relativity and Gravitation, Ch Experimental foundations: free fall, Lorentz invariance and clock tests

Problem

A Mössbauer source is mounted at the top of a cathedral spire of height h=62.0h = 62.0 m and the absorber at the bottom. Take g=9.81 m s−2g = 9.81\ \mathrm{m\,s^{-2}} as uniform over the spire and over the flight described below, and c=2.998×108 m s−1c = 2.998\times 10^{8}\ \mathrm{m\,s^{-1}}. All shifts are to be computed to first order in Φ/c2\Phi/c^2 and in v2/c2v^2/c^2. Separately, a caesium clock is flown on a research aircraft along a north-south meridian route at a constant ground speed u=250 m s−1u = 250\ \mathrm{m\,s^{-1}} and a constant altitude 11.011.0 km above the airfield, for an elapsed time of 8.008.00 h as read by the clock left at the airfield. Work in a frame in which the airfield is at rest and ignore the Earth's rotation entirely; ignore the climb and descent. ((a)) Calculate the magnitude of the predicted fractional frequency shift ∣Δν/ν∣|\Delta\nu/\nu| of the gamma rays received at the bottom of the spire. ((b)) Calculate the upward source speed that would exactly compensate this shift by a first-order Doppler shift. ((c)) Calculate the predicted reading difference (flown clock minus airfield clock) in ns at the end of the flight, and state whether it agrees with a measured value of +29±7+29 \pm 7 ns. ((d)) Name the pillar of the Einstein equivalence principle that the spire measurement tests, and the pillar that the velocity term of the flight comparison tests.

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