2017
DOI: 10.1016/j.ifacol.2017.08.2205
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Modeling and control of a Magnus effect-based airborne wind energy system in crosswind maneuvers

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Cited by 11 publications
(19 citation statements)
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“…As presented in [8], the dynamic equations of a Magnus cylinder can be derived in the cylinder's body frame, and then transferred to an inertial frame centered at the ground station through the application of rotation matrices. The position vector of the Magnus cylinder in the body frame r b is given by…”
Section: A System Modelmentioning
confidence: 99%
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“…As presented in [8], the dynamic equations of a Magnus cylinder can be derived in the cylinder's body frame, and then transferred to an inertial frame centered at the ground station through the application of rotation matrices. The position vector of the Magnus cylinder in the body frame r b is given by…”
Section: A System Modelmentioning
confidence: 99%
“…where S cyl refers to the projected surface area of the cylinder, v axz and v ay to the components of the apparent wind velocity, and C L and C D represent the coefficients of lift and drag, respectively. Still in accordance with [8], W b , F bu , and F r are used to denote the weight in the z b direction, the buoyancy force, and the tether traction force evaluated at the ground station, respectively. For the sake of simplicity, the tether dynamics is neglected, meaning that effects due to its drag, elasticity, and inertia are not considered.…”
Section: A System Modelmentioning
confidence: 99%
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