AIAA/AAS Astrodynamics Specialist Conference 2010
DOI: 10.2514/6.2010-8384
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Trans-Lunar Cruise Trajectory Design of GRAIL (Gravity Recovery and Interior Laboratory) Mission

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Cited by 15 publications
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“…Focusing on impulsive transfers, the complexity of these ranges from simple Hohmann transfers in a two-body model to weak stability boundary transfers with ballistic capture at the Moon in more complete astrodynamical models (Belbruno and Miller 1993;Hatch et al 2010). Particularly, an initial flyby at the Moon was proved to be a key feature to obtain an Earth-Moon transfer with a cost approaching the theoretical minimum of 3726 m/s, as estimated by Sweetser (1991).…”
Section: Introductionmentioning
confidence: 99%
“…Focusing on impulsive transfers, the complexity of these ranges from simple Hohmann transfers in a two-body model to weak stability boundary transfers with ballistic capture at the Moon in more complete astrodynamical models (Belbruno and Miller 1993;Hatch et al 2010). Particularly, an initial flyby at the Moon was proved to be a key feature to obtain an Earth-Moon transfer with a cost approaching the theoretical minimum of 3726 m/s, as estimated by Sweetser (1991).…”
Section: Introductionmentioning
confidence: 99%
“…The spacecraft performs small trajectory correction maneuvers, but otherwise coasts ballistically during the transfer. The GRAIL mission 1,2,3 is implementing a low-energy transfer 4 that is operationally similar to the direct transfer; that is, it involves a large maneuver to depart the Earth, a large maneuver to insert into orbit at the Moon, and a ballistic coast. The transfer requires less fuel, given the same propulsion system, though it requires 2-3 additional months of transfer duration.…”
Section: Introductionmentioning
confidence: 99%
“…From there they perform a series of maneuvers to transition into their science orbit. 3 In order to compare the GRAIL trajectory with those surveyed in this paper, and with the Apollo transfer discussed above, each GRAIL spacecraft would have a velocity of approximately 2.30 km/s at an altitude of 100 km if they did not initiate their orbit insertion before that point. A hypothetical impulsive orbit insertion maneuver would require a ΔV of approximately 0.67 km/s to insert each spacecraft into similar circular 100-km lunar orbits.…”
Section: Introductionmentioning
confidence: 99%
“…Exploiting BC grants several benefits in terms of both cost reduction (Belbruno and Miller, 1993) and mission versatility (Belbruno and Carrico, 2000;Topputo and Belbruno, 2015), in general at the cost of longer transfer times (Circi and Teofilatto, 2001;Ivashkin, 2002). In the past, the BC mechanism was used to rescue Hiten (Belbruno and Miller, 1990), and to design insertion trajectories in lunar missions like SMART-1 (Racca et al, 2002) and GRAIL (Chung et al, 2010). In the near future, BepiColombo will exploit BC orbits to be weakly captured by Mercury (Benkhoff et al, 2021;Schuster and Jehn, 2014).…”
mentioning
confidence: 99%