H-theorem: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  No edit summary | ||
| Line 8: | Line 8: | ||
| :<math>\sigma = -k \sum_{i,j} \int C(f_i,f_j) \ln f_i d {\mathbf u}_i</math> | :<math>\sigma = -k \sum_{i,j} \int C(f_i,f_j) \ln f_i d {\mathbf u}_i</math> | ||
| where the function C() represents binary collisions. | |||
| At equilibrium, <math>\sigma = 0</math>. | At equilibrium, <math>\sigma = 0</math>. | ||
| ==See also== | ==See also== | ||
Revision as of 11:17, 22 August 2007
Boltzmann's H-theorem states that the entropy of a closed system can only increase in the course of time, and must approach a limit as time tends to infinity.
where is the entropy source strength, given by (Eq 36 Chap IX Ref. 2)
where the function C() represents binary collisions. At equilibrium, .
See also
References
- L. Boltzmann "", Wiener Ber. 63 pp. 275- (1872)
- Sybren R. De Groot and Peter Mazur "Non-Equilibrium Thermodynamics", Dover Publications