Hamilton equations
The Hamilton equations are a formulation of the equations of motion in classical mechanics.
Local formulation
Suppose U⊆ℝn is an open set, suppose I is an interval (representing time), and H:U×ℝn×I→ℝ is a smooth function. Then the equations
˙qj | =∂H∂pj(q(t),p(t),t), | (1) | ||
˙pj | =-∂H∂qj(q(t),p(t),t), | (2) |
are the Hamilton equations for the curve
(q,p)=(q1,…,qn,p1,…,pn):I→U×ℝn. |
Such a solution is called a bicharacteristic, and H is called a Hamiltonian function. Here we use classical notation; the qi’s represent the location of the particles, the pi’s represent the momenta of the particles.
Global formulation
Suppose P is a symplectic manifold with symplectic form ω and that H:P→ℝ
is a smooth function. Then XH, the Hamiltonian
vector field corresponding to H is determined by
dH=ω(XH,⋅). |
The most common case is when P is the cotangent bundle of a manifold Q
equipped with the canonical symplectic form ω=-dα,
where α is the Poincaré 1-form (http://planetmath.org/Poincare1Form). (Note that other authors may have different sign convention.) Then Hamilton’s equations are the equations for the flow of the vector field XH. Given a system of coordinates x1,…x2n on the manifold P, they can be written as follows:
˙xi=(XH)i(x1,…x2n,t) |
The relation with the former definition is that in canonical
local coordinates (qi,pj) for T∗Q, the flow of XH
is determined by equations (1)-(2).
Also, the following terminology is frequently encountered — the manifold P is known as the phase space, the manifold Q is known as the configuration space, and the product P×ℝ is known as state space.
Title | Hamilton equations |
---|---|
Canonical name | HamiltonEquations |
Date of creation | 2013-03-22 14:45:58 |
Last modified on | 2013-03-22 14:45:58 |
Owner | CWoo (3771) |
Last modified by | CWoo (3771) |
Numerical id | 9 |
Author | CWoo (3771) |
Entry type | Definition |
Classification | msc 53D05 |
Classification | msc 70H05 |
Related topic | Quantization |