Liouville's theorem: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs)  (New page: :<math>\frac{d\varrho}{dt}= \sum_{i=1}^{s} \left( \frac{\partial \varrho}{\partial q_i} \dot{q_i}+ \frac{\partial \varrho}{\partial p_i} \dot{p_i} \right) =0 </math>  where <math>\varrho</...) | Carl McBride (talk | contribs)  No edit summary | ||
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| '''Liouville's theorem''' is an expression of the conservation of volume of [[phase space]]: | |||
| :<math>\frac{d\varrho}{dt}= \sum_{i=1}^{s} \left( \frac{\partial \varrho}{\partial q_i} \dot{q_i}+ \frac{\partial \varrho}{\partial p_i} \dot{p_i} \right) =0 </math> | :<math>\frac{d\varrho}{dt}= \sum_{i=1}^{s} \left( \frac{\partial \varrho}{\partial q_i} \dot{q_i}+ \frac{\partial \varrho}{\partial p_i} \dot{p_i} \right) =0 </math> | ||
| where <math>\varrho</math> is a distribution function <math>\varrho(p,q)</math>, ''p'' is the generalised momenta and ''q'' are the   | where <math>\varrho</math> is a distribution function <math>\varrho(p,q)</math>, ''p'' is the generalised momenta and ''q'' are the   | ||
| generalised coordinates. | generalised coordinates. | ||
| ==References== | ==References== | ||
| [[category: statistical mechanics]] | [[category: statistical mechanics]] | ||
Revision as of 12:17, 3 August 2007
Liouville's theorem is an expression of the conservation of volume of phase space:
where is a distribution function , p is the generalised momenta and q are the generalised coordinates.