2016
DOI: 10.1016/j.automatica.2016.07.045
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Energy shaping for position and speed control of a wheeled inverted pendulum in reduced space

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Cited by 17 publications
(2 citation statements)
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“…, q n ] T ∈ R n is the position vector,q ∈ R n is the velocity vector, M(q) = M T (q) > 0 ∈ R n×m is the inertia matrix, C(q,q) is the coriolis and centripental forces vector, B(q) ∈ R n is the potential forces vector, G(q) ∈ R n×m is the input coupling matrix and u ∈ R m is the applied torque vector. In fact, there exist a variety of systems with the structure of Equation (3) such as quadrotor (Zheng, Zhu, Zuo, & Yan, 2015), wheeled inverted pendulum (Delgado & Kotyczka, 2016) and many other mechanical systems.…”
Section: Problem Statementmentioning
confidence: 99%
“…, q n ] T ∈ R n is the position vector,q ∈ R n is the velocity vector, M(q) = M T (q) > 0 ∈ R n×m is the inertia matrix, C(q,q) is the coriolis and centripental forces vector, B(q) ∈ R n is the potential forces vector, G(q) ∈ R n×m is the input coupling matrix and u ∈ R m is the applied torque vector. In fact, there exist a variety of systems with the structure of Equation (3) such as quadrotor (Zheng, Zhu, Zuo, & Yan, 2015), wheeled inverted pendulum (Delgado & Kotyczka, 2016) and many other mechanical systems.…”
Section: Problem Statementmentioning
confidence: 99%
“…A controllability analysis for the WIP kinematics is presented in [17] and filtering techniques to prevent the WIP leading to limit cycle while stabilizing are discussed in [18]. Recently, a nonlinear position and velocity stabilization controller using energy shaping technique has been proposed in [19], and modeling of the WIP as a linear system with time delays and its stabilization using an integral slide mode control may be found in [20]. A fairly detailed overview of the WIP modeling with various stabilization and tracking control techniques may be found in [7].…”
Section: Introductionmentioning
confidence: 99%