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 Lagrangia[classical 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 ...](_blank)
, 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
:
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
::
: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
::
: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
::
where the matrix
::
::
: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
::
: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
::
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