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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National Academy of Science of Ukraine
2013-05-01
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Series: | Symmetry, Integrability and Geometry: Methods and Applications |
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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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