1999
DOI: 10.1002/(sici)1521-3889(199902)8:2<135::aid-andp135>3.3.co;2-e
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Cited by 25 publications
(49 citation statements)
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“…This goes against the naive 'dragging of inertial frames' intuition [2,29,30]. The total angular difference after n full revolutions would then be 6) which is another quantity one might consider measuring.…”
Section: Two-clock Clock Effectsmentioning
confidence: 99%
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“…This goes against the naive 'dragging of inertial frames' intuition [2,29,30]. The total angular difference after n full revolutions would then be 6) which is another quantity one might consider measuring.…”
Section: Two-clock Clock Effectsmentioning
confidence: 99%
“…For the Kerr-Taub-NUT spacetime in the equatorial plane, the t-φ 2-metric coefficients are [31] g tt = −1 + 2W, g tφ = −2aW, g φφ = (r 2 + a 2 + 2 ) + 2a 2 which is independent of the gravitational constant G and the orbital radius r [4,5,30,34] and has a value of about 10 −7 s for the Earth. However, there are experimental difficulties that must be overcome before there is any hope of measuring this effect [9,10,35,36].…”
Section: Kerr-taub-nut Equatorial Planementioning
confidence: 99%
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“…Moreover, different possibilities connected both with the clock effect and the gravitational Sagnac effect have been considered [5], [6].…”
Section: Introductionmentioning
confidence: 99%
“…The general relativistic clock effect, as worked out in [1,2], is the difference in the orbital periods of two clocks moving in opposite directions along a circular equatorial orbit around a central rotating mass. It is not an easy task to derive the general effect within the framework of Einstein's theory of gravitation; in fact, for orbits of arbitrary inclination to the equatorial plane, the clock effect has been derived only for the case that the orbiting bodies describe spherical orbits of constant 'radius' [2].…”
Section: Introductionmentioning
confidence: 99%