Physics Notes - Herong's Tutorial Notes - v3.25, by Herong Yang
What Is Poisson Bracket
This section provides a quick introduction to Poisson Bracket, which is an operation of two functions on the phase space (q,p) of a system.
What Is Poisson Bracket? Poisson Bracket is a partial differential expression of two functions on the phase space. Assuming that f(qi, pi, t) and g(qi, pi, t) are 2 functions on the phase space, the Poisson bracket expression is denoted as {f, g} and defined as below:
We can also be viewed as the dot product of gradient vector of f and the symplectic gradient vector of g.
{f, g} = [∂f/∂q, ∂f/∂p] ∙ [∂g/∂p, -∂g/∂q]
Poisson Bracket expression has the following properties.
1. Identity - Poisson Bracket of the same function is an constant zero.
{ f, f } = 0 (PB.2)
2. Anticommutativity - Also called Antisymmetry.
{ f, g } = - { g, f } (PB.3)
3. Bilinearity
{ f, ag+bh } = a{ f, g } + b{ f, h } (PB.4) { af+bg, h } = a{ f, h } + b{ g, h } (PB.5) where: a and b are constants h is another function h(qi, pi, t) on the phase space
4. Leibniz's () Rule - Also called the Product Rule.
{ fg, h } = { f, h }g + f { g, h } (PB.6) { f, gh } = { f, g }h + g { f, h } (PB.7)
5. Jacobi Identity - The sum of the cyclic permutation of double Poisson brackets of three functions is zero.
{ f, {g, h} } + { g, {h, f} } + { h, {f, g} } = 0 (PB.8)
6. Fundamental Poisson Brackets - The Poisson brackets of the canonical coordinates themselves are called the fundamental Poisson brackets. It is assumed that generalized position coordinates (q1, q2, ..., qn) and generalized momentum coordinates (p1, p2, ..., pn) are independent. That is ∂qi/∂pj = 0 and ∂pi/∂qj = 0.
δij is called Kronecker Delta, which is defined as:
Table of Contents
Introduction of Frame of Reference
Introduction of Special Relativity
Time Dilation in Special Relativity
Length Contraction in Special Relativity
The Relativity of Simultaneity
Minkowski Spacetime and Diagrams
Introduction of Generalized Coordinates
Phase Space and Phase Portrait
Poisson Bracket and Hamilton Equations