By Jorge Cortes

ISBN-10: 3540441549

ISBN-13: 9783540441540

Nonholonomic structures are a frequent subject in different medical and advertisement domain names, together with robotics, locomotion and house exploration. This paintings sheds new mild in this interdisciplinary personality during the research of numerous features coming from numerous disciplines. the most objective is to demonstrate the concept that a greater figuring out of the geometric buildings of mechanical structures unveils new and unknown points to them, and is helping either research and layout to unravel status difficulties and establish new demanding situations. during this manner, separate parts of study reminiscent of Classical Mechanics, Differential Geometry, Numerical research or regulate concept are introduced jointly during this research of nonholonomic platforms.

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Extra info for Geometric Control and Numerical Aspects of Nonholonomic Systems

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Given any singular point, there is no leaf passing through it. Consequently, D is not a completely integrable codistribution, but it is partially integrable. 3 Lie groups and group actions A N important and ubiquitous structure appearing in Mechanics is that of a Lie group. We refer the reader to [163, 253] for details and examples related to the discussion of this section. 3 Lie groups and group actions 19 Let G be a group, that is, a set with an additional internal operation · : G×G −→ G, usually called multiplication, satisfying the following defining properties 1.

The relation between the spatial and body momenta is given by means of the coadjoint action. 6. The coadjoint action of G on g∗ is defined as the map CoAd : G × g∗ −→ g∗ given by CoAd(g, p) = (Adg−1 )∗ p = Te∗ Lg−1 (Tg∗−1 Rg p). The body momentum is related to the spatial momentum via ps = CoAdg pb . Lie groups are mathematical objects that have been, and still are, intensively studied in their own right. ) that many mechanical systems exhibit. Their presence will generally allow us to develop reduction methods to simplify the description of (and, in some cases, help integrate) the dynamics of the given mechanical system.

Q is called the Liouville 1-form. In local coordinates (q A , pA ) on T ∗ Q, it reads ΘQ = pA dq A . It has some nice properties, such as, for instance, β ∗ ΘQ = β, for any 1-form β on Q. It also allows us to define the 2-form ωQ = −dΘQ . Obviously, ωQ is closed. In addition, it is also nondegenerate, and therefore (T ∗ Q, ωQ ) is a symplectic manifold. It is called the canonical symplectic form on T ∗ Q. In local coordinates, one can see that ωQ = dq A ∧ dpA . In fact, every symplectic manifold is locally isomorphic to a cotangent bundle.

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Geometric Control and Numerical Aspects of Nonholonomic Systems by Jorge Cortes

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