For the canonical Poisson bracket, direct substitution of F=qi and F=pi givesThereforeThis expresses the bracket as a first-order derivative acting on F, with coefficients determined by G; it is the phase-space chain-rule form of the definition.
{qi,G}=∂pi∂G,{pi,G}=−∂qi∂G.
∑i∂qi∂F{qi,G}+∑i∂pi∂F{pi,G}=∑i(FqiGpi−FpiGqi)={F,G}.
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