Setting dramatically
changes the shape of the potential.
It becomes a Two Wells Potential.
This potential harbors two minima at = +1 and -1 (
) and
a maximum at
. The phase space portrait of the solution
of this problem is very different than that of the single well
problem.
Use ,
,
,
and
in the
code implementing the RK4 solution of Duffing Oscillator.
Check that the energy is conserved, i.e., constant, for each trajectory.