VARIATIONAL PRINCIPLES FOR LIE-POISSON AND HAMILTON-POINCARE EQUATIONS

被引:56
作者
Cendra, Hernan [1 ,2 ]
Marsden, Jerrold E. [3 ]
Pekarsky, Sergey [4 ]
Ratiu, Tudor S. [5 ]
机构
[1] Univ Nacl Sur, Dept Matemat, RA-8000 Bahia Blanca, Buenos Aires, Argentina
[2] Consejo Nacl Invest Cient & Tecn, RA-1033 Buenos Aires, DF, Argentina
[3] CALTECH, Pasadena, CA 91125 USA
[4] Moodys Investors Serv, New York, NY 10007 USA
[5] Ecole Polytech Fed Lausanne, Ctr Bernoulli, CH-1015 Lausanne, Switzerland
基金
瑞士国家科学基金会;
关键词
D O I
10.17323/1609-4514-2003-3-3-833-867
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
As is well-known, there is a variational principle for the Euler-Poincare equations on a Lie algebra g of a Lie group G obtained by reducing Hamilton's principle on G by the action of G by, say, left multiplication. The purpose of this paper is to give a variational principle for the Lie-Poisson equations on g*, the dual of g, and also to generalize this construction. The more general situation is that in which the original configuration space is not a Lie group, but rather a configuration manifold Q on which a Lie group G acts freely and properly, so that Q -> Q/G becomes a principal bundle. Starting with a Lagrangian system on TQ invariant under the tangent lifted action of G, the reduced equations on (TQ)/G, appropriately identified, are the Lagrange-Poincare equations. Similarly, if we start with a Hamiltonian system on T*Q, invariant under the cotangent lifted action of G, the resulting reduced equations on (T*Q)/G are called the Hamilton-Poincare equations. Amongst our new results, we derive a variational structure for the Hamilton-Poincare equations, give a formula for the Poisson structure on these reduced spaces that simplifies previous formulas of Montgomery, and give a new representation for the symplectic structure on the associated symplectic leaves. We illustrate the formalism with a simple, but interesting example, that of a rigid body with internal rotors.
引用
收藏
页码:833 / 867
页数:35
相关论文
共 23 条
[1]  
[Anonymous], 1986, THESIS U CALIFORNIA
[3]  
Arnold V. I., 1985, ENCY MATH SCI, V3
[4]  
Arnold V. I., 1969, USPEHI MAT NAUK, V24, P225, DOI DOI 10.1007/978-3-642-31031-7_16
[5]  
Arnold V.I., 1989, MATH METHODS CLASSIC
[6]   The Euler-Poincare equations and double bracket dissipation [J].
Bloch, A ;
Krishnaprasad, PS ;
Marsden, JE ;
Ratiu, TS .
COMMUNICATIONS IN MATHEMATICAL PHYSICS, 1996, 175 (01) :1-42
[7]   A NOTE ON HAMILTONS PRINCIPLE FOR PERFECT FLUIDS [J].
BRETHERTON, FP .
JOURNAL OF FLUID MECHANICS, 1970, 44 (OCT) :19-+
[8]  
Cendra H., 1987, Journal of Geometry and Physics, V4, P183, DOI 10.1016/0393-0440(87)90026-X
[9]   The Maxwell-Vlasov equations in Euler-Poincare form [J].
Cendra, H ;
Holm, DD ;
Hoyle, MJW ;
Marsden, JE .
JOURNAL OF MATHEMATICAL PHYSICS, 1998, 39 (06) :3138-3157
[10]  
Cendra H, 2001, MEM AM MATH SOC, V152, P1