2015 IEEE Metrology for Aerospace (MetroAeroSpace) 2015
DOI: 10.1109/metroaerospace.2015.7180653
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On geodesic deviation in Schwarzschild spacetime

Abstract: For metrology, geodesy and gravimetry in space, satellite based instruments and measurement techniques are used and the orbits of the satellites as well as possible deviations between nearby ones are of central interest. The measurement of this deviation itself gives insight into the underlying structure of the spacetime geometry, which is curved and therefore described by the theory of general relativity (GR). In the context of GR, the deviation of nearby geodesics can be described by the Jacobi equation that… Show more

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Cited by 8 publications
(14 citation statements)
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“…We now recall the derivation of the Newtonian deviation equation, see, e.g., Ref. [4] and references therein. For a given reference curve Y µ (t) that fulfills the equation of motion we construct a second curve X µ (t) = Y µ (t) + η µ (t) and introduce the deviation η.…”
Section: Newtonian Deviation Equationmentioning
confidence: 99%
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“…We now recall the derivation of the Newtonian deviation equation, see, e.g., Ref. [4] and references therein. For a given reference curve Y µ (t) that fulfills the equation of motion we construct a second curve X µ (t) = Y µ (t) + η µ (t) and introduce the deviation η.…”
Section: Newtonian Deviation Equationmentioning
confidence: 99%
“…The meaning of these parameters and their impact on the perturbed orbit was studied briefly in Ref. [4], and the analysis will be extended in section 4 in the context of the general relativistic results. Note that the only frequency appearing in the solution so far is the Keplerian frequency Ω K .…”
Section: Deviation From Circular Reference Curvesmentioning
confidence: 99%
“…Where E and L are constants of motion given by R. 3,4,10 The most general solution of the deviation equation (9) in a spherically symmetric and static spacetime was found by Fuchs.…”
Section: Geodesic Deviation In General Relativitymentioning
confidence: 99%
“…3 If we set the constants C (1,2,3,4) equal to zero, we get a perturbed orbit that has a radius r = R and azimuthal motion ϕ(s) = Φ(s) = Ωs. However, the polar motion is given by Since the polar motion has the same frequency as the azimuthal motion T = 2π/Ω we have ϕ(2π/Ω) = 2π and ϑ(2π/Ω) = ϑ(0).…”
Section: Pendulum Orbitsmentioning
confidence: 99%
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