2007
DOI: 10.1134/s000511790708005x
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Parametric control in the problem of spacecraft stabilization in the geomagnetic field

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Cited by 33 publications
(22 citation statements)
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“…where ⃗ P = Q⃗ ρ 0 , Q is the total satellite charge, ⃗ ρ 0 = Q −1 ∫ V σ⃗ ρ dV is the radius vector of the satellite center of charge relative to its center of mass C, σ is the density of charge distribution over the satellite volume, ⃗ ρ is the radius vector of the satellite element dV relative to its center of mass, For the stabilization of the programmed motion, one can try to use the approach suggested in [1] choosing the laws of variation of parameters ⃗ P and ⃗ I as the sum of two terms…”
Section: Control Torquesmentioning
confidence: 99%
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“…where ⃗ P = Q⃗ ρ 0 , Q is the total satellite charge, ⃗ ρ 0 = Q −1 ∫ V σ⃗ ρ dV is the radius vector of the satellite center of charge relative to its center of mass C, σ is the density of charge distribution over the satellite volume, ⃗ ρ is the radius vector of the satellite element dV relative to its center of mass, For the stabilization of the programmed motion, one can try to use the approach suggested in [1] choosing the laws of variation of parameters ⃗ P and ⃗ I as the sum of two terms…”
Section: Control Torquesmentioning
confidence: 99%
“…In the problem of satellite electrodynamic attitude stabilization [1], [2], [4], [6] it is required to generate the control torques providing the existence and the asymptotic stability of the satellite position in the König frame such that the equations (1) hold, and, moreover, the satellite angular velocity with respect to the König frame is equal to zero:…”
Section: Coordinate Systems and Programmed Motionmentioning
confidence: 99%
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