Английская Википедия:Canonical coordinates
Шаблон:Short description Шаблон:Multiple issues Шаблон:Classical mechanics 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 classical mechanics. A closely related concept also appears in quantum mechanics; see the Stone–von Neumann theorem and canonical commutation relations for details.
As Hamiltonian mechanics are generalized by symplectic geometry and canonical transformations are generalized by contact transformations, so the 19th century definition of canonical coordinates in classical mechanics may be generalized to a more abstract 20th century definition of coordinates on the cotangent bundle of a manifold (the mathematical notion of phase space).
Definition in classical mechanics
In classical mechanics, canonical coordinates are coordinates <math>q^i</math> and <math>p_i</math> in phase space that are used in the Hamiltonian formalism. The canonical coordinates satisfy the fundamental Poisson bracket relations:
- <math>\left\{q^i, q^j\right\} = 0 \qquad \left\{p_i, p_j\right\} = 0 \qquad \left\{q^i, p_j\right\} = \delta_{ij}</math>
A typical example of canonical coordinates is for <math>q^i</math> to be the usual Cartesian coordinates, and <math>p_i</math> to be the components of momentum. Hence in general, the <math>p_i</math> coordinates are referred to as "conjugate momenta".
Canonical coordinates can be obtained from the generalized coordinates of the Lagrangian formalism by a Legendre transformation, or from another set of canonical coordinates by a canonical transformation.
Definition on cotangent bundles
Canonical coordinates are defined as a special set of coordinates on the cotangent bundle of a manifold. They are usually written as a set of <math>\left(q^i, p_j\right)</math> or <math>\left(x^i, p_j\right)</math> with the xШаблон:'s or qШаблон:'s denoting the coordinates on the underlying manifold and the pШаблон:'s denoting the conjugate momentum, which are 1-forms in the cotangent bundle at point q in the manifold.
A common definition of canonical coordinates is any set of coordinates on the cotangent bundle that allow the canonical one-form to be written in the form
- <math>\sum_i p_i\,\mathrm{d}q^i</math>
up to a total differential. A change of coordinates that preserves this form is a canonical transformation; these are a special case of a symplectomorphism, which are essentially a change of coordinates on a symplectic manifold.
In the following exposition, we assume that the manifolds are real manifolds, so that cotangent vectors acting on tangent vectors produce real numbers.
Formal development
Given a manifold Шаблон:Mvar, a vector field Шаблон:Mvar on Шаблон:Mvar (a section of the tangent bundle Шаблон:Math) can be thought of as a function acting on the cotangent bundle, by the duality between the tangent and cotangent spaces. That is, define a function
- <math>P_X: T^*Q \to \mathbb{R}</math>
such that
- <math>P_X(q, p) = p(X_q)</math>
holds for all cotangent vectors Шаблон:Mvar in <math>T_q^*Q</math>. Here, <math>X_q</math> is a vector in <math>T_qQ</math>, the tangent space to the manifold Шаблон:Mvar at point Шаблон:Mvar. The function <math>P_X</math> is called the momentum function corresponding to Шаблон:Mvar.
In local coordinates, the vector field Шаблон:Mvar at point Шаблон:Mvar may be written as
- <math>X_q = \sum_i X^i(q) \frac{\partial}{\partial q^i}</math>
where the <math>\partial /\partial q^i</math> are the coordinate frame on Шаблон:Mvar. The conjugate momentum then has the expression
- <math>P_X(q, p) = \sum_i X^i(q)\; p_i</math>
where the <math>p_i</math> are defined as the momentum functions corresponding to the vectors <math>\partial /\partial q^i</math>:
- <math>p_i = P_{\partial /\partial q^i}</math>
The <math>q^i</math> together with the <math>p_j</math> together form a coordinate system on the cotangent bundle <math>T^*Q</math>; these coordinates are called the canonical coordinates.
Generalized coordinates
In Lagrangian mechanics, a different set of coordinates are used, called the generalized coordinates. These are commonly denoted as <math>\left(q^i, \dot{q}^i\right)</math> with <math>q^i</math> called the generalized position and <math>\dot{q}^i</math> the generalized velocity. When a Hamiltonian is defined on the cotangent bundle, then the generalized coordinates are related to the canonical coordinates by means of the Hamilton–Jacobi equations.
See also
- Linear discriminant analysis
- Symplectic manifold
- Symplectic vector field
- Symplectomorphism
- Kinetic momentum
- Complementarity (physics)
- Canonical quantization
- Canonical quantum gravity
References
- Шаблон:Cite book
- Ralph Abraham and Jerrold E. Marsden, Foundations of Mechanics, (1978) Benjamin-Cummings, London Шаблон:Isbn See section 3.2.
