Behavior of nearby synchronous rotations of a Poincaré–Hough satellite at low eccentricity (original) (raw)
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In general, consider a planetary satellite (see Fig. 1) whose circular orbit normal K is inclined by an inclination Satellite spin states evolve under the action of solid body torques and tidal forces. The tidal effects result in a damping i with respect to an invariable plane normal n , about which of fast spin rates and, ultimately, in the locking of the spin it precesses with a rate ϪȐ (in rad/year). For close planeinto what are known as Cassini states. The dynamical equations tary satellites, the invariable plane is the planet's equatorial for the satellite spin vector are derived, non-dimensionalized, plane, and the orbit precession is caused by the oblateness and discussed. The non-dimensional parameters that determine of the planet. In general, the invariable plane is the satelthe ultimate fate of the system are identified. A review of Cassini lite's Laplace plane in the three body system (Goldreich states is given, and then the effect of a permanent triaxial 1966a, Ward 1981). The satellite's spin angular momentum deformation on the evolution of the spin vector is explored. in the k direction is tilted by an obliquity with respect We find that for the parameter ranges of most real Solar System to its orbit-plane normal K. If the satellite is oblate, the satellites which have been despun to synchronous rotation, planet exerts a torque which attempts to cause a precession occupation of Cassini state 1 is the only possible endpoint. The of the spin axis about K. We will assume in what follows existence of a non-axially symmetric deformation destabilizes the higher obliquity Cassini state 2. We discuss the possibility that the satellite is in principal-axis rotation about its axis of tumbling occurring during the spin-down and argue that of maximum moment of inertia. Averaged around the satthis does not effect our basic conclusions. The non-occupancy ellite's orbit, this torque is given by ϪSC cos sin , where of Cassini state 2 (except for the Moon, for which state 1 C is the satellite's moment of inertia about the spin axis and does not exist) is not a function of initial conditions or spin configuration occupied at synchronous lock, as previously hypothesized.
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A fmt-order, semianalytical theory for the long-term motion of resonant satellites is presented. The theory is valid for all eccentricities and inclinations and for all commensurability ratios. The method allows the inclusion of all the zonal 2nd tesserd harmonics as well as lunisolar perturbations and radiation pressure. The method is applied to a synchronous satellite including only the J, and J, harmonics. Global, long-term solutions for this problem, eccentricity, argument of perigee, and inclination are obtained.
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The present paper is devoted to the investigation of sufficient conditions for the existence of periodic solutions in the vicinity of stationary motion of a charged satellite in elliptic orbit. Lorentz forces which result from the motion of a charged satellite relative to the magnetic field of the Earth are considered. An axial symmetry is assumed about the center of mass of the satellite. In addition to the Lorentz force the perturbation caused by gravitational and magnetic fields of the Earth are considered. The stationary solutions and periodic orbits close to them are obtained using the Lyapunov theorem of holomorphic integral. Numerical results are used to explain the periodic motion of a certain satellite. It is shown that the charge-to-mass ratio has a significant influence on the periodic motion of satellites.