Lagrange bracket

Lagrange brackets are certain expressions closely related to Poisson brackets that were introduced by Joseph Louis Lagrange in 1808–1810 for the purposes of mathematical formulation of classical mechanics, but unlike the Poisson brackets, have fallen out of use.

Definition

Suppose that (q1, , qn, p1, , pn) is a system of canonical coordinates on a phase space. If each of them is expressed as a function of two variables, u and v, then the Lagrange bracket of u and v is defined by the formula

Properties

is a canonical transformation, then the Lagrange bracket is an invariant of the transformation, in the sense that
Therefore, the subscripts indicating the canonical coordinates are often omitted.
represents the components of Ω, viewed as a tensor, in the coordinates u. This matrix is the inverse of the matrix formed by the Poisson brackets
of the coordinates u.

See also

References

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