Basic Hamiltonian mechanics - CERN
where dG is a total differential. This follows from Hamilton’s variational principle Pk dQk ‘ H1(Qk1PkJ)df- Ep), dqk — H(qk,pk,t)dr | = dGi\[k (26) OCR Output canonical is (qk,pk) and (Qk,Pk ). The necessary and sufficient condition for a transformation to be The form of the equations is preserved in transforming between co—ordinate systems
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