Abstract:
An orbital gravitational dipole is a rectilinear inextensible rod of negligibly small mass which
moves in a Newtonian gravitational field and to whose ends two point loads are fastened. The
gravitational dipole is mainly designed to produce artificial gravity in a neighborhood of one of
the loads. In the nominal operational mode on a circular orbit the gravitational dipole is located
along the radius vector of its center of mass relative to the Newtonian center of attraction.
The main purpose of this paper is to investigate nonlinear oscillations of the gravitational
dipole in a neighborhood of its nominal mode. The orbit of the center of mass is assumed to
be circular or elliptic with small eccentricity. Consideration is given both to planar and arbitrary
spatial deviations of the gravitational dipole from its position corresponding to the nominal
mode. The analysis is based on the classical Lyapunov and Poincaré methods and the methods
of Kolmogorov – Arnold – Moser (KAM) theory. The necessary calculations are performed using
computer algorithms. An analytic representation is given for conditionally periodic oscillations.
Special attention is paid to the problem of the existence of periodic motions of the gravitational
dipole and their Lyapunov stability, formal stability (stability in an arbitrarily high, but
finite, nonlinear approximation) and stability for most (in the sense of Lebesgue measure) initial
conditions.
This research was carried out within the framework of the state assignment (registration No. AAAAA20-120011690138-6) at the Ishlinskii Institute for Problems in Mechanics, RAS, and at the Moscow
Aviation Institute (National Research University).
\Bibitem{Mar21}
\by A. P. Markeev
\paper On the Dynamics of a Gravitational Dipole
\jour Rus. J. Nonlin. Dyn.
\yr 2021
\vol 17
\issue 3
\pages 247--261
\mathnet{http://mi.mathnet.ru/nd754}
\crossref{https://doi.org/10.20537/nd210301}
\scopus{https://www.scopus.com/record/display.url?origin=inward&eid=2-s2.0-85118616059}
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