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Analytically calculated post-Keplerian range and range-rate perturbations: the solar Lense-Thirring effect and BepiColombo

Abstract

We analytically calculate the time series for the perturbations Δρ(t), Δρ˙(t)\Delta\rho(t),~\Delta\dot\rho(t) induced by a general disturbing acceleration A\boldsymbol{A} on the mutual range ρ\rho and range-rate ρ˙\dot\rho of two test particles A, B\textrm{A},~\textrm{B} orbiting the same spinning body. We apply it to the general relativistic Lense-Thirring effect, due to the primary's spin S\boldsymbol{S}, and the classical perturbation arising from its quadrupole mass moment J2J_2 for arbitrary orbital geometries and orientation of the source's symmetry axis S^\boldsymbol{\hat{S}}. The Earth-Mercury range and range-rate are nominally affected by the Sun's gravitomagnetic field to the 10 m, 103 cm s110~\textrm{m},~10^{-3}~\textrm{cm s}^{-1} level, respectively, during the extended phase (2026-2028) of the forthcoming BepiColombo mission to Mercury whose expected tracking accuracy is of the order of 0.1 m, 2×104 cm s1\simeq 0.1~\textrm{m},~2\times 10^{-4}~\textrm{cm s}^{-1}. The competing signatures due to the solar quadrupole J2J_2^\odot, if modelled at the σJ2109\sigma_{J_2^\odot}\simeq 10^{-9} level of the latest planetary ephemerides INPOP17a, are nearly 10 times smaller than the relativistic gravitomagnetic effects. The position and velocity vectors r, v\mathbf{r},~\mathbf{v} of Mercury and Earth are changed by the solar Lense-Thirring effect by about 10 m, 1.5 m10~\textrm{m},~1.5~\textrm{m} and 103 cm s1, 105 cm s110^{-3}~\textrm{cm s}^{-1},~10^{-5}~\textrm{cm s}^{-1}, respectively, over 2 yr; neglecting such shifts may have an impact on long-term integrations of the inner solar system dynamics over Gyr\sim\textrm{Gyr} timescales.Comment: LaTex2e, 29 pages, 8 figures, no tables. Matching the version at press in Monthly Notices of the Royal Astronomical Society (MNRAS

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