Hamilton's Equations

The equations defined by

q^.=(partialH)/(partialp)
(1)
p^.=-(partialH)/(partialq),
(2)

where p^.=dp/dt and q^.=dq/dt is fluxion notation and H is the so-called Hamiltonian, are called Hamilton's equations. These equations frequently arise in problems of celestial mechanics.

The vector form of these equations is

q^._i=H_(p_i)(t,q,p)
(3)
p^._i=-H_(q_i)(t,q,p)
(4)

(Zwillinger 1997, p. 136; Iyanaga and Kawada 1980, p. 1005).

Another formulation related to Hamilton's equation is

 p=(partialL)/(partialq^.),
(5)

where L is the so-called Lagrangian.

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