2009
DOI: 10.2514/1.36470
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Experiments with Small Unmanned Helicopter Nose-Up Landings

Abstract: ENGINEERING NOTES are short manuscripts describing new developments or important results of a preliminary nature. These Notes should not exceed 2500 words (where a figure or table counts as 200 words). Following informal review by the Editors, they may be published within a few months of the date of receipt. Style requirements are the same as for regular contributions (see inside back cover).

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Cited by 14 publications
(8 citation statements)
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“…x _ y _ z T = quadrotor translational velocities in I , m∕s ξ x y z T = quadrotor positions in I , m ξ s x s y s z s T = ship positions in I , m τ τ ϕ τ θ τ ψ T = torques along quadrotor body axes, N ⋅ m χ mx , χ my , χ mz = state vectors of the reference models for Δx, Δy, and Δz dynamics, respectively χ mz1 = first component of the vector χ mz , m Ω p q r T = quadrotor rotational velocities in Q, deg ∕s ω w , ω E = sea wave and encounter wave frequencies, respectively, rad∕s ω 0R , ω 0ACC = peak frequencies of the ship heave motion and ship heave acceleration spectrums, respectively, rad∕s I. Introduction T HE research in the automation of unmanned aerial vehicles (UAVs) has evolved rapidly over the past decades, which is driven by their various applications ranging from military combat to civilian infrastructure inspection [1,2]. Moreover, compared to manned aircrafts, the UAVs are more suitable and expandable for dull, dirty, and dangerous missions [3].…”
Section: Nomenclaturementioning
confidence: 99%
“…x _ y _ z T = quadrotor translational velocities in I , m∕s ξ x y z T = quadrotor positions in I , m ξ s x s y s z s T = ship positions in I , m τ τ ϕ τ θ τ ψ T = torques along quadrotor body axes, N ⋅ m χ mx , χ my , χ mz = state vectors of the reference models for Δx, Δy, and Δz dynamics, respectively χ mz1 = first component of the vector χ mz , m Ω p q r T = quadrotor rotational velocities in Q, deg ∕s ω w , ω E = sea wave and encounter wave frequencies, respectively, rad∕s ω 0R , ω 0ACC = peak frequencies of the ship heave motion and ship heave acceleration spectrums, respectively, rad∕s I. Introduction T HE research in the automation of unmanned aerial vehicles (UAVs) has evolved rapidly over the past decades, which is driven by their various applications ranging from military combat to civilian infrastructure inspection [1,2]. Moreover, compared to manned aircrafts, the UAVs are more suitable and expandable for dull, dirty, and dangerous missions [3].…”
Section: Nomenclaturementioning
confidence: 99%
“…UAVs have been extensively studied in recent decades due to their extensive in military and civilian applications [1][2][3][4][5][6]. In most multirotor aerial vehicle configurations, rotors are located in the same plane and are symmetrically fixed on the airframe.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, many approaches have been proposed to improve the control performance during recent years, such as PID, feedback linearization, backstepping control, robust control, internal model control (IMC) and neural network control (Agus and Singgih, 2007;Cai et al, 2008;Chien et al, 2008;Douik, 2008;Ferruz et al, 2011;Gadewadikar et al, 2009;Sˇpinka et al, 2011;Zheng and Zhong, 2011). The PID control method has been widely used in SRUA systems for its simple control structure (Bayraktar and Feron, 2009). By linearizing several operating points of the flight envelope, the control parameters can be designed directly, but it is easily affected by the wind disturbance (Cai et al, 2009).…”
Section: Introductionmentioning
confidence: 99%