Phase space: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs)  (New page: Phase space is the means by which the mechanical problem is converted in to geometry. '''Phase space''', or <math>\Gamma</math>-space, is a Euclidean space in <math>2s</math> dimensions  (...) | Carl McBride (talk | contribs)  m (Added an internal link.) | ||
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| Phase space is the means by which  | '''Phase space''' is the name given to a coordinate-momentum space.  | ||
| It is the means by which a mechanical problem can be  converted in to a geometrical problem. | |||
| Phase space, sometimes written as  <math>\Gamma</math>-space, is an Euclidean space in <math>2s</math> dimensions   | |||
| (''i.e.'' <math>E^{2s}</math>), where <math>s</math> | (''i.e.'' <math>E^{2s}</math>), where <math>s</math> | ||
| is the number of degrees of freedom. | is the number of [[degree of freedom |degrees of freedom]]. | ||
| Thus  | Thus a description of a system in terms of positions and velocities | ||
| now becomes a point in phase space. Changes in  | now becomes a point in phase space (known as a ''phase point''). Changes in the system now trace out a trajectory | ||
| in phase space. | in phase space (known as a ''phase trajectory'').  | ||
| Two different phase trajectories cannot pass through the same phase point. | |||
| One important property of phase space is that, for a long period of time, the phase-trajectory | |||
| will spend an equal amount of time in equal volume elements. | |||
| ==See also== | |||
| *[[Liouville's theorem]] | |||
| *[[H-theorem]] | |||
| [[category: statistical mechanics]] | [[category: statistical mechanics]] | ||
Latest revision as of 14:50, 30 July 2008
Phase space is the name given to a coordinate-momentum space. It is the means by which a mechanical problem can be converted in to a geometrical problem. Phase space, sometimes written as -space, is an Euclidean space in dimensions (i.e. ), where is the number of degrees of freedom. Thus a description of a system in terms of positions and velocities now becomes a point in phase space (known as a phase point). Changes in the system now trace out a trajectory in phase space (known as a phase trajectory). Two different phase trajectories cannot pass through the same phase point. One important property of phase space is that, for a long period of time, the phase-trajectory will spend an equal amount of time in equal volume elements.