Explain Hamilton's equation of motion in terms of Poisson's brackets.
Answer
set of first-order, highly symmetrical equations describing the motion of a classical dynamical system, namely
"q\u0307_j =\\frac{ \u2202 H }{\u2202 pj}\\\\, \u1e57_j =\\frac{ -\u2202 H }{\u2202 qj };"
here qj (j = 1, 2,…) are generalized coordinates of the system, pj is the momentum conjugate to qj , and H is the Hamiltonian.
"[Q, P]=1"
For canonical.
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