Volume 5: 6th International Conference on Multibody Systems, Nonlinear Dynamics, and Control, Parts A, B, and C 2007
DOI: 10.1115/detc2007-34574
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Discrete Mechanics and Optimal Control for Constrained Multibody Dynamics

Abstract: This paper formulates the dynamical equations of mechanics subject to holonomic constraints in terms of the states and controls using a constrained version of the Lagrange-d’Alembert principle. Based on a discrete version of this principle, a structure preserving time-stepping scheme is derived. It is shown that this respect for the mechanical structure (such as a reliable computation of the energy and momentum budget, without numerical dissipation) is retained when the system is reduced to its minimal dimensi… Show more

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Cited by 14 publications
(12 citation statements)
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“…A variational discrete null space method is proposed in (Leyendecker et al 2008). See also (Leyendecker et al (2007)). A study of the -convergence of VI's to the corresponding continuum action functional and the convergence properties of the discrete trajectories to stationary points of the continuum problem is presented in Schmidt et al (2009).…”
Section: Variational Integrationmentioning
confidence: 98%
“…A variational discrete null space method is proposed in (Leyendecker et al 2008). See also (Leyendecker et al (2007)). A study of the -convergence of VI's to the corresponding continuum action functional and the convergence properties of the discrete trajectories to stationary points of the continuum problem is presented in Schmidt et al (2009).…”
Section: Variational Integrationmentioning
confidence: 98%
“…No other force and torque are applied to this tree-structured system; therefore, in (42), the last matrix reduces to ⎡ [1,2,3], where the absolute reparametrization q n = F(u n , q 00 ) is used instead of (11) here. The motion starts and ends at rest.…”
Section: Optimal Control Of a Rigid Body With Rotorsmentioning
confidence: 99%
“…Null space matrix: Using I 12 = I−m 1 1 ⊗m 1 1 −m 1 2 ⊗ m 1 2 , the relation between the angular velocities reads x 2 = I 11 ·x 1 +˙ 2 n 1 . With regard to (36), the null space matrix for the E pair is given by…”
Section: Planar Pairmentioning
confidence: 99%
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