Jarzynski equality

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The Jarzynski equality, also known as the work relation or non-equilibrium work relation was developed by Chris Jarzynski. According to this equality, the equilibrium Helmholtz energy function of a process, (\(A\)), can be reconstructed by averaging the external work, \(W\), performed in many non-equilibrium realizations of the process (Eq. 2a in [1]): \[\exp \left( \frac{-\Delta A}{k_BT}\right)= \left\langle \exp \left( \frac{-W}{k_BT} \right) \right\rangle\]

or can be trivially re-written as (Eq. 2b)

\[\Delta A = - k_BT \ln \left\langle \exp \left( \frac{-W}{k_BT} \right) \right\rangle \] where \(k_B\) is the Boltzmann constant and \(T\) is the temperature. The only assumption in the proof of this relation is that of a weak coupling between the system and the reservoir. More recently Jarzynski has re-derived this formula, dispensing with this assumption [2].

[edit] See also

[edit] References

  1. Chris Jarzynski "Nonequilibrium Equality for Free Energy Differences", Physical Review Letters 78 2690-2693 (1997)
  2. Chris Jarzynski "Nonequilibrium work theorem for a system strongly coupled to a thermal environment", Journal of Statistical Mechanics: Theory and Experiment P09005 (2004)

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