1998
DOI: 10.1016/s0093-6413(98)00071-8
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Strategies for three dimensional deployment of tethered satellites

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Cited by 20 publications
(6 citation statements)
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“…3c, d and 4c, d. In the However, as soon as the tension control causes the tether to retrieve from ρ = 1 to ρ = 0.01, we have that the length rate settles down to ρ ′ = 0, the pitch motion returns to the equilibrium, and the roll motion settles down to a sinusoidal oscillation of constant amplitude, corresponding to a limit cycle 4 . In this connection, an out-of-plane thrusting for the retrieval phase have been proposed for several authors to help stabilize this process 21,23,30,41 .…”
Section: Resultsmentioning
confidence: 99%
“…3c, d and 4c, d. In the However, as soon as the tension control causes the tether to retrieve from ρ = 1 to ρ = 0.01, we have that the length rate settles down to ρ ′ = 0, the pitch motion returns to the equilibrium, and the roll motion settles down to a sinusoidal oscillation of constant amplitude, corresponding to a limit cycle 4 . In this connection, an out-of-plane thrusting for the retrieval phase have been proposed for several authors to help stabilize this process 21,23,30,41 .…”
Section: Resultsmentioning
confidence: 99%
“…However, as soon as the tension control caused the tether to retrieve from ρ = 1 to ρ = 0.01, the length rate settled down to ρ = 0; the pitch motion returned to equilibrium; and the roll motion settled down to a sinusoidal oscillation of constant amplitude corresponding to a limit cycle [3]. In this connection, Banerjee and Kane [21], Xu et al [44], Fujii and Ishijima [23], Kumar and Pradeep [30] proposed an out-of-plane thrusting for the retrieval phase to help stabilize this process. Figure 9 shows the in-plane and out-of-plane motion paths of the subsatellite for the controlled quasi-periodic (Figure 9a,b) and chaotic (Figuere 9c,d) trajectories.…”
Section: Deployment and Retrieval Performancesmentioning
confidence: 99%
“…Misra and Modi [41] and Nixon [3] studied the coupled motion of deployment and retrieval under a length-rate control algorithm in a circular orbit. Kumar and Pradeep [30], Salazar and Prado [39] linearized the motion equations about the local vertical to derive linear feedback control laws for the three-dimensional dynamics from a circular orbit. In this case, Kumar and Pradeep [30] employed a combination of tension control and out-ofplane thrusting.…”
Section: Introductionmentioning
confidence: 99%
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“…Alternate control laws based on the linear regulator problem were developed by Bainum et al in 1980 (Bainum andKumar 1980). A linear tension control law was provided by Pradeep in 1998 (Kumar andPradeep 1998). In 1999, Pradhan, Modi, and Misra (1999) presented a paper which studied several applications of the offset scheme in controlling the tethered systems.…”
mentioning
confidence: 99%