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Entropic bounds on currents in Langevin systems.
Andreas Dechant1, Shin-Ichi Sasa1
1Department of Physics No. 1, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan.
Physical Review. E
|July 18, 2018
Summary
Generalized currents in Langevin systems are bounded by total entropy production. This entropic bound reveals power-efficiency tradeoffs for ratchets and heat engines, limiting maximum efficiency to zero power output.
Area of Science:
- Statistical Mechanics
- Non-equilibrium Thermodynamics
- Physical Chemistry
Background:
- Langevin systems describe the dynamics of particles influenced by random forces and friction.
- Entropy production quantifies irreversibility in thermodynamic processes.
- Ratchets and heat engines are devices that convert thermal energy into work.
Purpose of the Study:
- To derive a fundamental bound on generalized currents in Langevin systems.
- To investigate the implications of this bound for the efficiency of ratchets and heat engines.
- To explore constraints on irreversible currents and power-efficiency tradeoffs.
Main Methods:
- Derivation of a generalized current bound based on total entropy production.
- Analysis of overdamped and underdamped Langevin dynamics.
- Application of the bound to Smoluchowski-Feynman, flashing, and rocking ratchets.
- Examination of periodically driven heat engines and Onsager matrix constraints.
Main Results:
- Any generalized current in overdamped Langevin systems is bounded by the entropy production rate.
- This entropic bound leads to power-efficiency tradeoff relations for various ratchets.
- For underdamped dynamics, output power and heat absorption rate are bounded by entropy production.
- Power-efficiency tradeoffs are established for underdamped ratchets and driven heat engines.
Conclusions:
- The derived entropic bound provides fundamental limits on the performance of nanoscale engines.
- Power-efficiency tradeoffs are a general consequence of entropy production in driven systems.
- The study offers insights into the interplay between thermodynamics and dynamics in non-equilibrium systems.
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