Non-autonomous mechanics explained

Q\toR

over the time axis

R

coordinated by

(t,qi)

.

This bundle is trivial, but its different trivializations

Q=R x M

correspond to the choice of different non-relativistic reference frames. Such a reference frame also is represented by a connection

\Gamma

on

Q\toR

which takes a form

\Gammai=0

with respect to this trivialization. The corresponding covariant differential
i)\partial
(q
i
determines the relative velocity with respect to a reference frame

\Gamma

.

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

X=R

. Accordingly, the velocity phase space of non-autonomous mechanics is the jet manifold

J1Q

of

Q\toR

provided with the coordinates

(t,qi,q

i
t)
. Its momentum phase space is the vertical cotangent bundle

VQ

of

Q\toR

coordinated by
i,p
(t,q
i)
and endowed with the canonical Poisson structure. The dynamics of Hamiltonian non-autonomous mechanics is defined by a Hamiltonian form
i-H(t,q
p
idq
i,p
i)dt
.

One can associate to any Hamiltonian non-autonomous system an equivalent Hamiltonian autonomous system on the cotangent bundle

TQ

of

Q

coordinated by
i,p,p
(t,q
i)
and provided with the canonical symplectic form; its Hamiltonian is

p-H

.

See also

References