2010
DOI: 10.1007/s00332-010-9078-6
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Nonlinear Dynamics of the 3D Pendulum

Abstract: A 3D pendulum consists of a rigid body, supported at a fixed pivot, with three rotational degrees of freedom. The pendulum is acted on by a gravitational force. 3D pendulum dynamics have been much studied in integrable cases that arise when certain physical symmetry assumptions are made. This paper treats the nonintegrable case of the 3D pendulum dynamics when the rigid body is asymmetric and the center of mass is distinct from the pivot location. 3D pendulum full and reduced models are introduced and used to … Show more

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Cited by 46 publications
(24 citation statements)
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“…In this section, we implement the derived structure linearization on two examples: the asymmetric 3D pendulum [22]- [25] and the quadrotor with a suspended load [26]- [28], which synthesizes the current analysis and control tools. Both systems have been studied extensively by the robotic community and various controllers have been designed by exploring the system dynamics.…”
Section: Methodsmentioning
confidence: 99%
“…In this section, we implement the derived structure linearization on two examples: the asymmetric 3D pendulum [22]- [25] and the quadrotor with a suspended load [26]- [28], which synthesizes the current analysis and control tools. Both systems have been studied extensively by the robotic community and various controllers have been designed by exploring the system dynamics.…”
Section: Methodsmentioning
confidence: 99%
“…First, we develop a second-order method based on the trapezoidal rule for a free-flying body that is able to undergo arbitrarily large rotations and displacements in space. This problem has been extensively studied from both theoretical and numerical aspects (see, e.g., Meyer et al 2009;Bauchau and Bottasso 1999;Chaturvedi et al 2011;Lee et al 2007;Marsden and Ratiu 1999;Simo and Wong 1991) among others) since its configuration space corresponds to a nonlinear differentiable manifold rather than a linear space. The second example corresponds to the formulation of an explicit, second-order accurate varitational integrator for finite element discretizations of geometrically exact rods.…”
Section: Final Examplesmentioning
confidence: 99%
“…It follows that the function V is positive-definite and decrescent. Choose any initial state (R(0), Ω(0)) satisfying (23). By (15) in Lemma III.4, V 0 (R(t), Ω(t), t) is a non-increasing function of time along the closed-loop trajectory and (24) holds for all t ≥ 0, which implies…”
Section: Consider a Lyapunov Function (Candidate)mentioning
confidence: 99%