Liouville's theorem (Hamiltonian)
:A separate article is about Liouville's theorem in complex analysis: see Liouville's theorem (complex analysis).
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In mathematical physics, Liouville's theorem, named after the French mathematician Joseph Liouville, is a key theorem in classical statistical and Hamiltonian mechanics. It asserts that the phase-space distribution function is constant along the trajectories of the system - that is that the density of system points in the vicinity of a given system point travelling through phase-space is constant with time..
Related Topics:
Mathematical physics - Joseph Liouville - Statistical - Hamiltonian mechanics - Phase-space
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Liouville's theorem is also important in the study of symplectic topology, where it is formulated rather differently.
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~ Table of Content ~
| ► | Introduction |
| ► | Liouville equation |
| ► | Physical interpretation |
| ► | Other formulations |
| ► | See also |
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