Relative Critical Points

Relative equilibria of Lagrangian and Hamiltonian systems with symmetry are critical points of appropriate scalar functions parametrized by the Lie algebra (or its dual) of the symmetry group. Setting aside the structures – symplectic, Poisson, or variational – generating dynamical systems from such...

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Main Author: Debra Lewis
Format: Article
Language:English
Published: National Academy of Science of Ukraine 2013-05-01
Series:Symmetry, Integrability and Geometry: Methods and Applications
Subjects:
Online Access:http://dx.doi.org/10.3842/SIGMA.2013.038
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spelling doaj-1a5da92c81654c8cadb00234c06938702020-11-24T23:39:40ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592013-05-01903810.3842/SIGMA.2013.038Relative Critical PointsDebra LewisRelative equilibria of Lagrangian and Hamiltonian systems with symmetry are critical points of appropriate scalar functions parametrized by the Lie algebra (or its dual) of the symmetry group. Setting aside the structures – symplectic, Poisson, or variational – generating dynamical systems from such functions highlights the common features of their construction and analysis, and supports the construction of analogous functions in non-Hamiltonian settings. If the symmetry group is nonabelian, the functions are invariant only with respect to the isotropy subgroup of the given parameter value. Replacing the parametrized family of functions with a single function on the product manifold and extending the action using the (co)adjoint action on the algebra or its dual yields a fully invariant function. An invariant map can be used to reverse the usual perspective: rather than selecting a parametrized family of functions and finding their critical points, conditions under which functions will be critical on specific orbits, typically distinguished by isotropy class, can be derived. This strategy is illustrated using several well-known mechanical systems – the Lagrange top, the double spherical pendulum, the free rigid body, and the Riemann ellipsoids – and generalizations of these systems.http://dx.doi.org/10.3842/SIGMA.2013.038relative equilibriasymmetriesconservative systemsRiemann ellipsoids
collection DOAJ
language English
format Article
sources DOAJ
author Debra Lewis
spellingShingle Debra Lewis
Relative Critical Points
Symmetry, Integrability and Geometry: Methods and Applications
relative equilibria
symmetries
conservative systems
Riemann ellipsoids
author_facet Debra Lewis
author_sort Debra Lewis
title Relative Critical Points
title_short Relative Critical Points
title_full Relative Critical Points
title_fullStr Relative Critical Points
title_full_unstemmed Relative Critical Points
title_sort relative critical points
publisher National Academy of Science of Ukraine
series Symmetry, Integrability and Geometry: Methods and Applications
issn 1815-0659
publishDate 2013-05-01
description Relative equilibria of Lagrangian and Hamiltonian systems with symmetry are critical points of appropriate scalar functions parametrized by the Lie algebra (or its dual) of the symmetry group. Setting aside the structures – symplectic, Poisson, or variational – generating dynamical systems from such functions highlights the common features of their construction and analysis, and supports the construction of analogous functions in non-Hamiltonian settings. If the symmetry group is nonabelian, the functions are invariant only with respect to the isotropy subgroup of the given parameter value. Replacing the parametrized family of functions with a single function on the product manifold and extending the action using the (co)adjoint action on the algebra or its dual yields a fully invariant function. An invariant map can be used to reverse the usual perspective: rather than selecting a parametrized family of functions and finding their critical points, conditions under which functions will be critical on specific orbits, typically distinguished by isotropy class, can be derived. This strategy is illustrated using several well-known mechanical systems – the Lagrange top, the double spherical pendulum, the free rigid body, and the Riemann ellipsoids – and generalizations of these systems.
topic relative equilibria
symmetries
conservative systems
Riemann ellipsoids
url http://dx.doi.org/10.3842/SIGMA.2013.038
work_keys_str_mv AT debralewis relativecriticalpoints
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