Abstract:
In this study, we concluded the Hamiltonian equations on (ℳ9
, λ,XH) , being a model. Finally introduce, some geometrical and
physical results on the related mechanic systems have been discussed. n classical mechanics we can describe the state of a system by
specifying its Lagrangian as a function of the coordinates and their time rates of change. Hamilton realized that Lagrange’s equations of
motion were equivalent to a variational principle.