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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. T ...
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 In mathematics and classical mechanics, canonical coordinates are sets of coordinates on phase space which can be used to describe a physical system at any given point in time. Canonical coordinates are used in the Hamiltonian formulation of c ...
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 usual ...
. 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 In mathematics and classical mechanics, canonical coordinates are sets of coordinates on phase space which can be used to describe a physical system at any given point in time. Canonical coordinates are used in the Hamiltonian formulation of c ...
(''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. Canon ...
, 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 U or u, is the twenty-first and sixth-to-last letter and fifth vowel letter of the Latin alphabet, used in the modern English alphabet, the alphabets of other western European languages and others worldwide. Its name in English is ''u'' (pro ...
, \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 tens ...
, in the coordinates ''u''. This matrix is the
inverse Inverse or invert may refer to: Science and mathematics * Inverse (logic), a type of conditional sentence which is an immediate inference made from another conditional sentence * Additive inverse (negation), the inverse of a number that, when ad ...
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) ''momen ...


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 He or HE may refer to: Language * He (pronoun), an English pronoun * He (kana), the romanization of the Japanese kana へ * He (letter), the fifth letter of many Semitic alphabets * He (Cyrillic), a letter of the Cyrillic script called ''He'' ...
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