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Nonequilibrium work relations for systems subject to mechanical and thermal changes.

Riccardo Chelli1

  • 1Dipartimento di Chimica, Università di Firenze, Via della Lastruccia 3, I-50019 Sesto Fiorentino, Italy. chelli@chim.unifi.it

The Journal of Chemical Physics
|February 12, 2009
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Summary

This study generalizes the Crooks fluctuation theorem for Hamiltonian and non-Hamiltonian systems undergoing mechanical and thermal changes. It extends nonequilibrium work relations, offering a unified framework for statistical mechanics research.

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Area of Science:

  • Statistical Mechanics
  • Non-equilibrium Thermodynamics
  • Physical Chemistry

Background:

  • The Crooks fluctuation theorem is crucial for understanding non-equilibrium processes.
  • Existing formulations often focus on specific system types (e.g., Hamiltonian).
  • A generalized approach is needed to encompass broader physical systems.

Purpose of the Study:

  • To derive generalized forms of the Crooks fluctuation theorem.
  • To extend its applicability to both Hamiltonian and non-Hamiltonian systems.
  • To unify derivations for mechanical and thermal changes.

Main Methods:

  • Derivations based on the Liouville equation.
  • Assumption of stationary probability distribution for fixed parameters and temperature.
  • Application to systems with isochoric-isokinetic and isothermal-isobaric equations of motion.

Main Results:

  • Generalized Crooks fluctuation theorem derived for diverse systems.
  • Identical derivations for Hamiltonian and non-Hamiltonian cases.
  • Extended several key non-equilibrium work relations (Jarzynski equality, Bennett acceptance ratio, etc.).

Conclusions:

  • The generalized theorem provides a unified framework for non-equilibrium statistical mechanics.
  • The methodology is broadly applicable and extends to other work theorems.
  • Demonstrates applicability through illustrative examples in thermodynamics.