Hamiltonian canonical equations of motion for a conservation system are

\frac{- d q _{i}}{d t} = \frac{\partial H}{\partial P _{i}} and \frac{- d P _{i}}{d t} = \frac{\partial H}{\partial q _{i}}

\frac{d q _{i}}{d t} = \frac{\partial H}{\partial P _{i}} and \frac{d P _{i}}{d t} = \frac{\partial H}{\partial q _{i}}

\frac{- d q _{i}}{d t} = \frac{\partial H}{\partial P _{i}} and \frac{d P _{i}}{d t} = \frac{\partial H}{\partial q _{i}}

\frac{d q _{i}}{d t} = \frac{\partial H}{\partial P _{i}} and \frac{- d P _{i}}{d t} = \frac{\partial H}{\partial q _{i}}

Answer

Answer: Option D

Answer: Option D

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