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On the geometric approach to the motion of inertial mechanical systems

REVIEW ARTICLE

Adrian Constantin1 and Boris Kolev2

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TOPICAL REVIEW

According to the principle of least action, the spatially periodic motions of one-dimensional mechanical systems with no external forces are described in the Lagrangian formalism by geodesics on a manifold-configuration space, the group Script D of smooth orientation-preserving diffeomorphisms of the circle. The periodic inviscid Burgers equation is the geodesic equation on Script D with the L2 right-invariant metric. However, the exponential map for this right-invariant metric is not a C1 local diffeomorphism and the geometric structure is therefore deficient. On the other hand, the geodesic equation on Script D for the H1 right-invariant metric is also a re-expression of a model in mathematical physics. We show that in this case the exponential map is a C1 local diffeomorphism and that if two diffeomorphisms are sufficiently close on Script D, they can be joined by a unique length-minimizing geodesic—a state of the system is transformed to another nearby state by going through a uniquely determined flow that minimizes the energy. We also analyse for both metrics the breakdown of the geodesic flow.


PACS

45.10.Na Geometrical and tensorial methods

02.30.Jr Partial differential equations

02.40.Vh Global analysis and analysis on manifolds

MSC

70Hxx Hamiltonian and Lagrangian mechanics (See also 37Jxx)

70S05 Lagrangian formalism and Hamiltonian formalism

53Axx Classical differential geometry

Subjects

Mathematical physics

Computational physics

Dates

Issue 32 (16 August 2002)

Received 31 May 2002, in final form 19 June 2002

Published 2 August 2002



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