Lagrange Bracket
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Lagrange brackets are certain expressions closely related to
Poisson bracket In mathematics and classical mechanics, the Poisson bracket is an important binary operation in Hamiltonian mechanics, playing a central role in Hamilton's equations of motion, which govern the time evolution of a Hamiltonian dynamical system. Th ...
s that were introduced by
Joseph Louis Lagrange Joseph-Louis Lagrange (born Giuseppe Luigi Lagrangiaclassical mechanics Classical mechanics is a physical theory describing the motion of macroscopic objects, from projectiles to parts of machinery, and astronomical objects, such as spacecraft, planets, stars, and galaxies. For objects governed by classical ...
, but unlike the Poisson brackets, have fallen out of use.


Definition

Suppose that (''q''1, …, ''q''''n'', ''p''1, …, ''p''''n'') is a system of canonical coordinates on a
phase space In dynamical system theory, a phase space is a space in which all possible states of a system are represented, with each possible state corresponding to one unique point in the phase space. For mechanical systems, the phase space usually ...
. 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 = \sum_^n \left(\frac \frac - \frac \frac \right).


Properties

* Lagrange brackets do not depend on the system of canonical coordinates (''q'', ''p''). If (''Q'',''P'') = (''Q''1, …, ''Q''''n'', ''P''1, …, ''P''''n'') is another system of canonical coordinates, so that :: Q=Q(q,p), P=P(q,p) :is a
canonical transformation In Hamiltonian mechanics, a canonical transformation is a change of canonical coordinates that preserves the form of Hamilton's equations. This is sometimes known as form invariance. It need not preserve the form of the Hamiltonian itself. Canoni ...
, then the Lagrange bracket is an invariant of the transformation, in the sense that :: u, v = , v :Therefore, the subscripts indicating the canonical coordinates are often omitted. * If ''Ω'' is the
symplectic form In mathematics, a symplectic vector space is a vector space ''V'' over a field ''F'' (for example the real numbers R) equipped with a symplectic bilinear form. A symplectic bilinear form is a mapping that is ; Bilinear: Linear in each argument ...
on the ''2n''-dimensional phase space ''W'' and ''u''''1'',…,''u''''2n'' form a system of coordinates on ''W'', the symplectic form can be written as :: \Omega = \frac 12 \Omega_ du^i \wedge du^j where the matrix :: \Omega_ = u_i, u_j , \quad 1\leq i,j\leq 2n :: :represents the components of , viewed as a
tensor In mathematics, a tensor is an algebraic object that describes a multilinear relationship between sets of algebraic objects related to a vector space. Tensors may map between different objects such as vectors, scalars, and even other tenso ...
, in the coordinates ''u''. This matrix is the inverse of the matrix formed by the Poisson brackets :: \left(\Omega^\right)_ = \, \quad 1 \leq i,j \leq 2n :of the coordinates ''u''. * As a corollary of the preceding properties, coordinates (''Q''1, ..., ''Q''''n'', ''P''1, …, ''P''''n'') on a phase space are canonical if and only if the Lagrange brackets between them have the form :: _i, Q_j=0, \quad _i,P_j=0,\quad _i, P_j=- _j, Q_i=\delta_.


See also

*
Lagrangian mechanics In physics, Lagrangian mechanics is a formulation of classical mechanics founded on the stationary-action principle (also known as the principle of least action). It was introduced by the Italian-French mathematician and astronomer Joseph-Lou ...
*
Hamiltonian mechanics Hamiltonian mechanics emerged in 1833 as a reformulation of Lagrangian mechanics. Introduced by Sir William Rowan Hamilton, Hamiltonian mechanics replaces (generalized) velocities \dot q^i used in Lagrangian mechanics with (generalized) ''momenta ...


References

*
Cornelius Lanczos __NOTOC__ Cornelius (Cornel) Lanczos ( hu, Lánczos Kornél, ; born as Kornél Lőwy, until 1906: ''Löwy (Lőwy) Kornél''; February 2, 1893 – June 25, 1974) was a Hungarian-American and later Hungarian-Irish mathematician and physicist. Accor ...
, ''The Variational Principles of Mechanics'', Dover (1986), . * Iglesias, Patrick, ''Les origines du calcul symplectique chez Lagrange'' he origins of symplectic calculus in Lagrange's work L'Enseign. Math. (2) 44 (1998), no. 3-4, 257–277.


External links

* * {{SpringerEOM, author=A.P. Soldatov, title=Lagrange bracket Bilinear maps Hamiltonian mechanics