Non-autonomous mechanics explained
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
.
See also
References
- De Leon, M., Rodrigues, P., Methods of Differential Geometry in Analytical Mechanics (North Holland, 1989).
- Echeverria Enriquez, A., Munoz Lecanda, M., Roman Roy, N., Geometrical setting of time-dependent regular systems. Alternative models, Rev. Math. Phys. 3 (1991) 301.
- Carinena, J., Fernandez-Nunez, J., Geometric theory of time-dependent singular Lagrangians, Fortschr. Phys., 41 (1993) 517.
- Mangiarotti, L., Sardanashvily, G., Gauge Mechanics (World Scientific, 1998) .
- Giachetta, G., Mangiarotti, L., Sardanashvily, G., Geometric Formulation of Classical and Quantum Mechanics (World Scientific, 2010) .