University Physics Notes: Classical Mechanics – Time Dependent Canonical Transformations
Time dependent canonical transformations are very similar to the
time independent case, and as with the time independent case, the
preservation of area is a part of the analysis. Consider the
transformation
The
condition for such a transformation to preserve Hamiltonian form is
that the Jacobian is a non zero constant.
Suppose therefore that
not
necessarily Hamiltonian, is transformed to
where![]()
The Jacobian will depend explicitly on the time in general and in
terms of the new coordinates
we
have![]()
If in the original coordinates
the
system is Hamiltonian then
and![]()
From this it can be deduced that for Hamiltonian form to be
preserved we must have![]()
The properties of generating functions are carried over from the
time independent case, though now the generating function are now
also functions of time, with a generating function being determined
up to the addition of a function of time alone. The relations between
the generating functions and the old and new variables remain the
same. For a generating function![]()
For all the generating functions,
up
to the addition of a function of time,![]()
For example,![]()
![]()
But
and
so![]()