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


[ u, v ]_{p,q} = \sum_{i=1}^n \left(\frac{\partial q_i}{\partial u} \frac{\partial p_i}{\partial v} - \frac{\partial p_i}{\partial u} \frac{\partial q_i}{\partial v} \right).

Properties

 Q=Q(q,p), P=P(q,p)
is a canonical transformation, then the Lagrange bracket is an invariant of the transformation, in the sense that
 [ u, v]_{q,p} = [u , v]_{Q,P}
Therefore, the subscripts indicating the canonical coordinates are often omitted.
 [ u_i, u_j ]_{p,q}, \quad 1\leq i,j\leq 2n
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
 \{u_i, u_j\}, \quad 1\leq i,j\leq 2n
of the coordinates u.
 [Q_i, Q_j]_{p,q}=0, \quad [P_i,P_j]_{p,q}=0,\quad [Q_i, P_j]_{p,q}=-[P_j, Q_i]_{p,q}=\delta_{ij}.

See also

References

External links

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