# Difference between revisions of "H-theorem"

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#[http://store.doverpublications.com/0486647412.html Sybren R. De Groot and Peter Mazur "Non-Equilibrium Thermodynamics", Dover Publications] | #[http://store.doverpublications.com/0486647412.html Sybren R. De Groot and Peter Mazur "Non-Equilibrium Thermodynamics", Dover Publications] | ||

#[http://www.oup.com/uk/catalogue/?ci=9780195140187 Robert Zwanzig "Nonequilibrium Statistical Mechanics", Oxford University Press (2001)] | #[http://www.oup.com/uk/catalogue/?ci=9780195140187 Robert Zwanzig "Nonequilibrium Statistical Mechanics", Oxford University Press (2001)] | ||

+ | '''Related reading''' | ||

+ | *[http://dx.doi.org/10.1073/pnas.1001185107 Philip T. Gressman and Robert M. Strain "Global classical solutions of the Boltzmann equation with long-range interactions", Proceedings of the National Academy of Sciences of the United States of America '''107''' pp. 5744-5749 (2010)] | ||

+ | |||

[[category: non-equilibrium thermodynamics]] | [[category: non-equilibrium thermodynamics]] |

## Revision as of 11:01, 19 May 2010

## Contents

## Boltzmann's H-theorem

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, .

## Boltzmann's H-function

Boltzmann's *H-function* is defined by (Eq. 5.66 Ref. 3):

where is the molecular velocity. A restatement of the H-theorem is

## Gibbs's H-function

## See also

## References

- L. Boltzmann "", Wiener Ber.
**63**pp. 275- (1872) - Sybren R. De Groot and Peter Mazur "Non-Equilibrium Thermodynamics", Dover Publications
- Robert Zwanzig "Nonequilibrium Statistical Mechanics", Oxford University Press (2001)

**Related reading**