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نویسندگان مقالات پربازدید :
اخترفیزیک و علوم فضایی 2013
جزئیات رویداد
همایش ، رویداد ، ژورنال
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  • on the construction of low-energy cislunar and translunar transfers based on the libration points

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    • تاریخ ارائه: 1392/07/24
    • تاریخ انتشار در تی پی بین: 1392/07/24
    • تعداد بازدید: 1083
    • تعداد پرسش و پاسخ ها: 0
    • شماره تماس دبیرخانه رویداد: -
     there exist cislunar and translunar libration points near the moon, which are referred to as the ll 1and ll 2 points, respectively. they can generate the different types of low-energy trajectories transferring from earth to moon. the time-dependent analytic model including the gravitational forces from the sun, earth, and moon is employed to investigate the energy-minimal and practical transfer trajectories. however, different from the circular restricted three-body problem, the equivalent gravitational equilibria are defined according to the geometry of the instantaneous hill boundary due to the gravitational perturbation from the sun. the relationship between the altitudes of periapsis and eccentricities is achieved from the poincaré mapping for all the captured lunar trajectories, which presents the statistical feature of the fuel cost and captured orbital elements rather than generating a specified moon-captured segment. the minimum energy required by the captured trajectory on a lunar circular orbit is deduced in the spatial bi-circular model. the idea is presented that the asymptotical behaviors of invariant manifolds approaching to/traveling from the libration points or halo orbits are destroyed by the solar perturbation. in fact, the energy-minimal cislunar transfer trajectory is acquired by transiting the ll 1 point, while the energy-minimal translunar transfer trajectory is obtained by transiting the ll 2 point. finally, the transfer opportunities for the practical trajectories that have escaped from the earth and have been captured by the moon are yielded by the transiting halo orbits near the ll 1 and ll 2 points, which can be used to generate the whole of the trajectories.

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