This paper considers systems subject to nonholonomic constraints which are not uniform on the whole configuration manifold. When the constraints change, the system undergoes a transition in order to comply with the new imposed conditions. Building on previous work on the Hamiltonian theory of impact, we tackle the problem of mathematically describing the classes of transitions that can occur. We propose a comprehensive formulation of the transition principle that encompasses the various impulsive regimes of Hamiltonian systems. Our formulation is based on the partial symplectic formalism, which provides a suitable framework for the dynamics of nonholonomic systems. We pay special attention to mechanical systems and illustrate the results with several examples.
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April 2006
Research Article|
April 28 2006
Hamiltonian theory of constrained impulsive motion Available to Purchase
Jorge Cortés;
Jorge Cortés
a)
Department of Applied Mathematics and Statistics, Baskin School of Engineering,
University of California
, Santa Cruz, California 95064
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Alexandre M. Vinogradov
Alexandre M. Vinogradov
b)
Dipartimento di Matematica e Informatica,
Università di Salerno and Istituto Nazionale di Fisica Nucleare
, Via S. Allende, I-84081 Baronissi, Italy
Search for other works by this author on:
Jorge Cortés
a)
Department of Applied Mathematics and Statistics, Baskin School of Engineering,
University of California
, Santa Cruz, California 95064
Alexandre M. Vinogradov
b)
Dipartimento di Matematica e Informatica,
Università di Salerno and Istituto Nazionale di Fisica Nucleare
, Via S. Allende, I-84081 Baronissi, Italya)
Electronic mail: [email protected]
b)
Electronic mail: [email protected]
J. Math. Phys. 47, 042905 (2006)
Article history
Received:
October 05 2005
Accepted:
March 15 2006
Citation
Jorge Cortés, Alexandre M. Vinogradov; Hamiltonian theory of constrained impulsive motion. J. Math. Phys. 1 April 2006; 47 (4): 042905. https://doi.org/10.1063/1.2192974
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