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Poisson brackets | Identities of Poisson brackets | Classical Mechanics

Poisson brackets and its identities

Poisson brackets

  • A Poisson bracket is a special kind of relation between a pair of dynamical variables of any holonomic system, which is found to remain invariant under any canonical transformation.
  • They are used to construct new integrals of motion from the known integrals.
  • They are classical analogues of commutation relation between operators in quantum mechanics.
  • If u (p, q, t) and v (p, q, t) are two dynamical variables, then the Poisson bracket of these quantities with respect to canonical variables (p, q) is
                

Identities of Poisson brackets

  • [u, v] = – [v, u]


  • Thus the Poisson bracket of any two dynamical variables is anti-commutative.
  • If u = v, then
                
  • [u, u](p, q) = 0
  • [uu] = [vv] = 0

  • If c is any constant, then [cu, v] = [u, cv] = c [u, v]

  • Similarly [u, cv] = c [u, v]
  • ∴  [cu, v] = [u, cv] = c [u, v]

  • The Poisson brackets satisfy the distributive property
  • [u + v, w] = [u, w] + [v, w] and [u, v w] = [u, v]w + v[u, w]

  • Similarly [u, v w] = [u, v]w + v[u, w]

  • The partial derivative of Poisson bracket is

  • Jacobi identity of Poisson bracket is [u [v, w]] + [v [w, u]] + [w [u, v]] = 0

  • If F (w1, w2, …, wn) be a differentiable function of w1, w2, …, wn and all w’s be the function of (p, q, t), then

  • Let F (w1, w2) be a differentiable function of w1 and w2

To know about Poisson bracket and its identities please click on the link for English and  click on the link for Hindi

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