2008
DOI: 10.2514/1.33616
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Nonlinear Dynamic Equations of Satellite Relative Motion Around an Oblate Earth

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Cited by 85 publications
(29 citation statements)
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“…Therefore, based on the desired crosstrack velocity, the argument of latitude at which the burn must occur can be calculated based on Eq. (22). In this scenario, the first burn should occur immediately and the following burns should occur at the argument of latitude which produces the desired crosstrack motion.…”
Section: Initial Burnmentioning
confidence: 99%
“…Therefore, based on the desired crosstrack velocity, the argument of latitude at which the burn must occur can be calculated based on Eq. (22). In this scenario, the first burn should occur immediately and the following burns should occur at the argument of latitude which produces the desired crosstrack motion.…”
Section: Initial Burnmentioning
confidence: 99%
“…Therefore, the time of the burn, or θ 0 , can be chosen, so that Eq. (22) are not violated and a circular projection is still achieved. In this example it is likely that the burn will be non-equatorial.…”
Section: A Effects Of Crosstrack Motionmentioning
confidence: 99%
“…The Hill-Clohessy-Wiltshire (HCW) equation cannot be used for high-fidelity modeling and simulation due to its assumptions on linearization, circular orbit, and no perturbation. The high-fidelity nonlinear dynamic models for the reference (chief) and relative motions with both the J 2 perturbation and atmospheric drag were presented by either hybrid states [19] or the classical orbital parameters [21], based on [22]. We present some key attributes of swarm dynamics based on these new models.…”
Section: A Swarm Orbital Dynamics Under J 2 and Atmospheric Dragmentioning
confidence: 99%