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 group reports three separate measurements. Throughout, take the local free-fall acceleration at the site as g=9.81ms−2 and c=2.998×108ms−1. All accelerations, heights and elapsed times below are quoted in the Earth (laboratory) frame, and air resistance is ignored throughout. Use the first-order gravitational rate results of this chapter, that is, work to first order in gh/c2.
((a)) An aluminium mass and a copper mass are released in the laboratory and fall with accelerations g1=9.8120040ms−2 and g2=9.8120036ms−2. Compute the Eötvös parameter η.
((b)) Gamma rays are emitted by a source at the foot of a tower of height 30.0m and received by a detector at the top. Compute the predicted magnitude of the fractional frequency shift ∣Δν∣/ν between emission and reception.
((c)) An atomic clock is carried in an aircraft that circles at a constant altitude of 9.00km above a ground station for 36.0h of ground-clock time, and is then compared with the clock that stayed at the station. Ignore all velocity effects and Earth's rotation, and use only the first-order gravitational rate difference gh/c2. (i) Predict, to the nearest nanosecond, the reading of the flown clock minus the reading of the ground clock. (ii) The measured offset is (138±15)ns. By how many nanoseconds (nearest nanosecond) does the measured value differ from your prediction?