Phase space: Difference between revisions
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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 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. Changes in the system now trace out a trajectory | ||
in phase space. | in phase space. | ||
One of the most important properties 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]] |
Revision as of 11:41, 3 August 2007
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. Changes in the system now trace out a trajectory in phase space.
One of the most important properties 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.