Canonical equations
In classical mechanics, the canonical equations are the equations of motion of a system that is described by a Hamilton function, and are therefore also called Hamilton's equations of motion . They are
- and
Mean
- the generalized coordinates
- the generalized impulses of the system.
The canonical equations follow directly from Hamilton's principle through an extended variation principle , in which coordinates and impulses are treated equally.
The canonical equations are closely linked to the canonical transformations that bridge the gap to quantum mechanics via the Hamilton-Jacobi equation . The elegant formulation of the canonical equations with Poisson brackets provides a first indication of this :
- and
For any phase space function of the system one can write the total derivative with respect to time as:
- ,
for a detailed derivation of this notation see Poisson brackets #Hamilton's equation of motion .
This form shows the correspondence between the classical equation of motion of a phase space function and Heisenberg's equation of motion for observables in quantum mechanics.
literature
- Herbert Goldstein; Charles P. Poole, Jr; John L. Safko: Classical Mechanics . 3. Edition. Wiley-VCH, Weinheim 2006, ISBN 3-527-40589-5 .
- Wolfgang Nolting: Basic Course Theoretical Physics 2 Analytical Mechanics . 7th edition. Springer, Heidelberg 2006, ISBN 3-540-30660-9 .
- Wolfgang Nolting: Basic Course Theoretical Physics 5/1 Quantum Mechanics Basics . 6th edition. Springer, Heidelberg 2004, ISBN 3-540-40071-0 .