Non-autonomous mechanics describe non-relativistic mechanical systems subject to time-dependent transformations. In particular, this is the case of mechanical systems whose Lagrangians and Hamiltonians depend on the time. The configuration space of non-autonomous mechanics is a fiber bundle over the time axis coordinated by .
This bundle is trivial, but its different trivializations correspond to the choice of different non-relativistic reference frames. Such a reference frame also is represented by a connection
on which takes a form with respect to this trivialization. The corresponding covariant differential
determines the relative velocity with respect to a reference frame .
As a consequence, non-autonomous mechanics (in particular, non-autonomous Hamiltonian mechanics) can be formulated as a covariant classical field theory (in particular covariant Hamiltonian field theory) on . Accordingly, the velocity phase space of non-autonomous mechanics is the jet manifold of provided with the coordinates . Its momentum phase space is the vertical cotangent bundle of coordinated by and endowed with the canonical Poisson structure. The dynamics of Hamiltonian non-autonomous mechanics is defined by a Hamiltonian form .
One can associate to any Hamiltonian non-autonomous system an equivalent Hamiltonian autonomous system on the cotangent bundle of coordinated by and provided with the canonical symplectic form; its Hamiltonian is .
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Non-autonomous mechanics describe non-relativistic mechanical systems subject to time-dependent transformations. In particular, this is the case of mechanical systems whose Lagrangians and Hamiltonians depend on the time. The configuration space of non-autonomous mechanics is a fiber bundle over the time axis coordinated by . This bundle is trivial, but its different trivializations correspond to the choice of different non-relativistic reference frames.
La mécanique analytique est une formulation de la mécanique classique basée sur le calcul variationnel. La mécanique analytique s'est avérée un outil très important en physique théorique. En particulier, la mécanique quantique emprunte énormément au formalisme de la mécanique analytique. Contrairement à la mécanique d'Isaac Newton qui s'appuie sur le concept de point matériel, la mécanique analytique se penche sur les systèmes arbitrairement complexes, et étudie l'évolution de leurs degrés de libertés dans ce qu'on appelle un espace de configuration.