Free-energy difference from nonequilibrium work
Equilibrium free-energy difference
For a system at fixed inverse temperature (with the temperature ) and control parameter , the equilibrium Helmholtz free energy is
where is the canonical partition function (compare Helmholtz free energy and statistical free energy ).
The equilibrium free-energy difference between endpoints of a protocol is
Nonequilibrium identification via work statistics
Even if the protocol is fast and drives the system out of equilibrium, is determined by nonequilibrium work fluctuations:
Jarzynski estimator
If realizations start in equilibrium at and work is measured (see work distribution ), then
which is exactly Jarzynski’s equality rewritten as a formula for .
Crooks crossing / likelihood methods
If both forward and reverse experiments are available, the Crooks fluctuation theorem
implies:
- Crossing method: solve to get .
- Likelihood-based estimation: infer from the full set of observed forward/reverse work samples (statistically efficient in practice).
Dissipation and information
Define dissipated work . Then (by Jensen) is a nonequilibrium refinement of the second law and can be related to a relative entropy between forward and reverse path ensembles (a path-space irreversibility measure).
Practical cautions
- The Jarzynski exponential average can be dominated by rare low-work events, leading to slow convergence for finite samples.
- Using reverse data (Crooks-based inference) often reduces variance compared to forward-only estimation.