Hamilton equations
The Hamilton equations are a formulation of the equations of motion in classical mechanics.
Local formulation
Suppose is an open set, suppose is an interval (representing time), and is a smooth function. Then the equations
| (1) | ||||
| (2) |
are the Hamilton equations for the curve
Such a solution is called a bicharacteristic, and is called a Hamiltonian function. Here we use classical notation; the ’s represent the location of the particles, the ’s represent the momenta of the particles.
Global formulation
Suppose is a symplectic manifold![]()
with symplectic form and that
is a smooth function. Then , the Hamiltonian
vector field corresponding to is determined by
The most common case is when is the cotangent bundle of a manifold![]()
equipped with the canonical symplectic form ,
where is the Poincaré -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 . Given a system of coordinates on the manifold , they can be written as follows:
The relation![]()
with the former definition is that in canonical
local coordinates for , the flow of
is determined by equations (1)-(2).
Also, the following terminology is frequently encountered — the manifold is known as the phase space, the manifold is known as the configuration space, and the product 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 |