- ...distance
- Important point: dy is entirely independent of
y!
Think of it as a step of size , which can be chosen
arbitrarily,
with no relation to the place from which you step.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...functional
- L can contain t explicitly if the
potential V is time-dependent. We ignore this in the following.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...equation.
- Since Hamilton instructs us to
solve a boundary value problem, with and fixed, the
variation is fixed to be zero at and .
Thus x in (33) is not a boundary point, and there
are no boundary terms to worry about.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...solution.
- Just change the boundary conditions on
, for example.
A more interesting alternative is to add
to the energy (50).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.