Crooks fluctuation theorem: Difference between revisions
		
		
		
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| The '''Crooks fluctuation theorem''' was developed by Gavin E. Crooks. It is also known as the ''Crooks Identity'' or the ''Crooks fluctuation relation''. | The '''Crooks fluctuation theorem''' was developed by Gavin E. Crooks. It is also known as the ''Crooks Identity'' or the ''Crooks fluctuation relation''. It is given by (Ref. 1 Eq. 2): | ||
| :<math>\frac{P_F( | |||
| :<math>\frac{P_F(+\omega)}{P_R(-\omega)}= \exp({+ \omega})</math> | |||
| where <math>\omega</math> is the [[entropy]] production, <math>P_F(\omega)</math> is the "forward" probability distribution of this entropy production, and <math>P_R(-\omega)</math>, time-reversed. This expression can be written in  terms of [[work]] (<math>W</math>) (Ref. 1 Eq. 11): | |||
| :<math>\frac{P_F(+\beta W)}{P_R(- \beta W)}= \exp (- \Delta A) \exp (+\beta W)</math> | |||
| where <math>\beta := 1/(k_BT)</math> where <math>k_B</math> is the [[Boltzmann constant]] and <math>T</math> is the [[temperature]], and <math>A</math> is the [[Helmholtz energy function]]. | |||
| ==References== | ==References== | ||
| #[http://dx.doi.org/10.1103/PhysRevE.60.2721  Gavin E. Crooks  "Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences", Physical Review E '''60''' pp. 2721 - 2726 (1999)] | #[http://dx.doi.org/10.1103/PhysRevE.60.2721  Gavin E. Crooks  "Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences", Physical Review E '''60''' pp. 2721 - 2726 (1999)] | ||
| [[category:Non-equilibrium thermodynamics]] | [[category:Non-equilibrium thermodynamics]] | ||
| [[category: fluctuation theorem]] | [[category: fluctuation theorem]] | ||
Revision as of 11:53, 6 February 2008
The Crooks fluctuation theorem was developed by Gavin E. Crooks. It is also known as the Crooks Identity or the Crooks fluctuation relation. It is given by (Ref. 1 Eq. 2):
where  is the entropy production,  is the "forward" probability distribution of this entropy production, and , time-reversed. This expression can be written in  terms of work () (Ref. 1 Eq. 11):
where  where  is the Boltzmann constant and  is the temperature, and  is the Helmholtz energy function.
