<p>Uncontrolled geostationary satellites abandoned near an unstable equilibrium point of the equator experience irregular transitions between dynamical states (continuous circulation, long and short libration). They are caused by the interaction between the longitudinal dynamics, governed by the tesseral harmonics of the geopotential, and the orbital precession forced by Earth’s oblateness and lunisolar perturbations. The transitions are extremely sensitive to small perturbations, making the long-term evolution unpredictable. Recently, a Monte Carlo analysis of trajectories starting at the <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(165^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>165</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>E unstable equilibrium point, revealed that the evolution to chaos is not gradual. It occurs via sudden episodes of disorder at specific points of the precession cycle, when the orbital inclination is minimal. Due to the high cost of the statistical analysis, the results where limited to a single initial longitude. This paper applies modified versions of the diameter Lagrangian descriptor to reduce the computational burden. This enables mapping the dynamical behavior over the complete range of longitudes where transitions between modes of motion are possible, encompassing both unstable equilibrium points (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(165^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>165</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>E and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(15^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>15</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>W). It is found that the episodes of chaos remain linked to the orbital inclination cycle, but their timing depends on the initial spacecraft longitude. As the initial position moves farther away from the unstable points, the transitions take place at higher values of the orbital inclination. The longitudes where the transitions occur at maximum inclination correspond to the boundaries of the chaotic region.</p>

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Uncontrolled geostationary satellites: mapping periodic transitions to chaos with Lagrangian Descriptors

  • R. Flores,
  • J. Daquin,
  • M. Pontani,
  • H. Susanto,
  • E. Fantino

摘要

Uncontrolled geostationary satellites abandoned near an unstable equilibrium point of the equator experience irregular transitions between dynamical states (continuous circulation, long and short libration). They are caused by the interaction between the longitudinal dynamics, governed by the tesseral harmonics of the geopotential, and the orbital precession forced by Earth’s oblateness and lunisolar perturbations. The transitions are extremely sensitive to small perturbations, making the long-term evolution unpredictable. Recently, a Monte Carlo analysis of trajectories starting at the \(165^\circ \) 165 E unstable equilibrium point, revealed that the evolution to chaos is not gradual. It occurs via sudden episodes of disorder at specific points of the precession cycle, when the orbital inclination is minimal. Due to the high cost of the statistical analysis, the results where limited to a single initial longitude. This paper applies modified versions of the diameter Lagrangian descriptor to reduce the computational burden. This enables mapping the dynamical behavior over the complete range of longitudes where transitions between modes of motion are possible, encompassing both unstable equilibrium points ( \(165^\circ \) 165 E and \(15^\circ \) 15 W). It is found that the episodes of chaos remain linked to the orbital inclination cycle, but their timing depends on the initial spacecraft longitude. As the initial position moves farther away from the unstable points, the transitions take place at higher values of the orbital inclination. The longitudes where the transitions occur at maximum inclination correspond to the boundaries of the chaotic region.