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100 Years of Relativity Space-Time Structure: Einstein and Beyond ...

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260 N. Ashbyflawed technical report 1 was issued as late as 1996 by an apparently authoritativesource–the Aerospace Corporation, where the civilian counterpart <strong>of</strong>the JPO is located. One source <strong>of</strong> confusion was the Sagnac effect thatmakes it impossible to self-consistently synchronize clocks on the surface<strong>of</strong> the rotating earth by performing operations with electromagnetic signalsor slowly moving portable clocks, like those that could successfully beused to synchronize clocks in an inertial frame. Thus a problem that hadto be solved was effective synchronization <strong>of</strong> clocks fixed or slowly movingon earth’s surface. Another source <strong>of</strong> confusion was whether the sun’sgravitational potential would have a significant effect on clocks in GPSsatellites.The GPS is made possible by extremely accurate, stable atomic clocks.Figure 1 gives a plot <strong>of</strong> the Allan deviation σ y (τ) for a high-performanceCesium clock, as a function <strong>of</strong> sample time τ. If an ensemble <strong>of</strong> clocks isinitially synchronized, then when compared to each other after a time τ, theAllan deviation provides a measure <strong>of</strong> the rms fractional frequency deviationamong the clocks due to intrinsic noise processes in the clocks. Frequency<strong>of</strong>fsets <strong>and</strong> frequency drifts are additional systematic effects which must beaccounted for separately. Also on Figure 1 is an Allan deviation plot for aQuartz oscillator such as is typically found in a GPS receiver. Quartz oscillatorsusually have better short-term stability performance characteristicsthan Cesium clocks, but after <strong>100</strong> seconds or so, Cesium has far betterperformance. In actual clocks there is a wide range <strong>of</strong> variation around thenominal values plotted in Figure 1. The most stable GPS clocks use Rubidiumatoms <strong>and</strong> reach maximum stability levels <strong>of</strong> a few parts in 10 15 afterabout ten days. What this means is that after initializing such a clock, <strong>and</strong>leaving it alone for ten days, it should be correct to within about 5 partsin 10 15 , or 0.4 nanoseconds. Relativistic effects are huge compared to this.The purpose <strong>of</strong> this article is to explain how relativistic effects are accountedfor in the GPS. Although clock velocities are small <strong>and</strong> gravitationalfields are weak near the earth, they give rise to significant relativisticeffects. These effects include first- <strong>and</strong> second-order Doppler frequencyshifts <strong>of</strong> clocks due to their relative motion, gravitational frequencyshifts, <strong>and</strong> the Sagnac effect due to earth’s rotation. If such effects are notaccounted for properly, unacceptably large errors in GPS navigation <strong>and</strong>time transfer will result. In the GPS one can find many examples <strong>of</strong> theapplication <strong>of</strong> fundamental relativity principles. Also, experimental tests <strong>of</strong>relativity can be performed with GPS, although generally speaking theseare not at a level <strong>of</strong> precision any better than previously existing tests.

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