2016
DOI: 10.1002/rnc.3554
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Finite-time angular velocity observers for rigid-body attitude tracking with bounded inputs

Abstract: The attitude tracking of a rigid body without angular velocity measurements is addressed. A continuous angular velocity observer with fractional power functions is proposed to estimate the angular velocity via quaternion attitude information. The fractional power gains can be properly tuned according to a homogeneous method such that the estimation error system is uniformly almost globally finite-time stable, irrespective of control inputs. To achieve output feedback attitude tracking control, a quaternion-bas… Show more

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Cited by 55 publications
(50 citation statements)
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“…If α 1 = α 2 = 1, controller (8) becomes u = À k 1 e 0 e v À k 2 sat(ω e /p 2 (t)) + u d , which ensures uniform almost global asymptotic stability of Z 0 , as shown in [25]. In addition, the nontrivial unstable equilibria are…”
Section: Remarkmentioning
confidence: 96%
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“…If α 1 = α 2 = 1, controller (8) becomes u = À k 1 e 0 e v À k 2 sat(ω e /p 2 (t)) + u d , which ensures uniform almost global asymptotic stability of Z 0 , as shown in [25]. In addition, the nontrivial unstable equilibria are…”
Section: Remarkmentioning
confidence: 96%
“…Because initial conditions convergent to the unstable equilibria iI3Zi form a subset of measure zero, the probability of entering such a set is zero, and for practical purposes, this possibility can be ignored. Moreover, perturbations such as external disturbances can drive the spacecraft attitude away from the unstable equilibria.Remark If α 1 = α 2 = 1, controller (8) becomes u = − k 1 e 0 e v − k 2 sat( ω e / p 2 ( t )) + u d , which ensures uniform almost global asymptotic stability of Z0, as shown in . In addition, the nontrivial unstable equilibria are Z4={}(),eboldωeS3×3:boldeQ0.1em4,ωe=0, where Q0.1em4={}boldeS3:‖‖boldev=1.…”
Section: Control Design With Integral Terminal Sliding Modementioning
confidence: 98%
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