The ARTEMIS Mission 2012
DOI: 10.1007/978-1-4614-9554-3_4
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ARTEMIS Mission Design

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Cited by 11 publications
(14 citation statements)
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“…The Halo orbit from which the spacecraft is departing is chosen to have a z−excursion of 5000 km around the EM libration point L 2 , see Figure 3. The choice for this specific Halo orbit is motivated by the successful Artemis mission [22,23] During the period represented in Figure 1, asteroid 2006RH 120 does 17 clockwise revolutions around the origin of the CR3BP frame, and 3.6 revolutions in Earth inertial reference frame. The evolution of the energy of 2006RH 120 and its distance to the Earth-Moon libration point L 2 as the asteroid evolves on its orbit are given in Figure 4.…”
Section: Rendezvous To 2006rh 120mentioning
confidence: 99%
See 1 more Smart Citation
“…The Halo orbit from which the spacecraft is departing is chosen to have a z−excursion of 5000 km around the EM libration point L 2 , see Figure 3. The choice for this specific Halo orbit is motivated by the successful Artemis mission [22,23] During the period represented in Figure 1, asteroid 2006RH 120 does 17 clockwise revolutions around the origin of the CR3BP frame, and 3.6 revolutions in Earth inertial reference frame. The evolution of the energy of 2006RH 120 and its distance to the Earth-Moon libration point L 2 as the asteroid evolves on its orbit are given in Figure 4.…”
Section: Rendezvous To 2006rh 120mentioning
confidence: 99%
“…Rendezvous missions to asteroids in the inner solar system can be found in [10,17] but they concern asteroids on elliptic orbits which is not the case for us since TCOs are presenting complex orbits and therefore require a different methodology. Our assumption on the hibernating location for the spacecraft, a Halo orbit around the Earth-Moon unstable Libration points L 2 , is motivated in part from the successful Artemis mission [22,23] and in part from the constraint on the duration of the mission, mostly impacted by the time of detection of the asteroid. Indeed, the Arthemis mission demonstrated low delta-v (∆v) station keeping on Halo orbits around L 1 and L 2 .…”
Section: Introductionmentioning
confidence: 99%
“…For example, if the motion of the satellite is limited in the planet-moonmoon system, such as the Saturn-Tethys-Telesto-spacecraft, Saturn-Tethys-Calypso-spacecraft, and Saturn-Dione-Helenspacecraft systems, they are typical R4BP systems. If the motion of the satellite is limited in the planet-moon system while the Sun's gravitational influence cannot be neglected, such as ARTEMIS mission [1], the system needs to be modeled as the R4BP as well. Meanwhile, for the mission exploring the Sun-planet system, such as GALA and PLANCK [2], the R3BP model is suitable when we consider the Sun and the barycenter of the planet and its moon as two dominant masses move around their center of mass along either circular or elliptic orbits.…”
Section: Introductionmentioning
confidence: 99%
“…to a planetary flyby, in which case a two body approximation is sufficient for mission design purposes). This is the case of libration point (LP) missions, for which dynamical systems techniques were introduced relatively recently and are now widely spread [7,8,10,11,14,22]. Genesis [14] has been the first LP mission to make use of a heteroclinic connection between objects related to the L 1 and L 2 points of the Sun-Earth system.…”
Section: Introductionmentioning
confidence: 99%
“…Genesis [14] has been the first LP mission to make use of a heteroclinic connection between objects related to the L 1 and L 2 points of the Sun-Earth system. More recently, Artemis [22] has also used heteroclinic connections between the L 1 and L 2 dynamics but in the Earth-Moon system, with a more complex final trajectory. The trajectories of these two missions are shown in Figure 1.…”
Section: Introductionmentioning
confidence: 99%