H-theorem: Difference between revisions
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:<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 12:17, 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.
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma \geq 0}
where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma} is the entropy source strength, given by (Eq 36 Chap IX Ref. 2)
where the function C() represents binary collisions. At equilibrium, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma = 0} .
See also
References
- L. Boltzmann "", Wiener Ber. 63 pp. 275- (1872)
- Sybren R. De Groot and Peter Mazur "Non-Equilibrium Thermodynamics", Dover Publications