Thermodynamics in finite time. I. The step-Carnot cycle

Bjarne Andresen, R. Stephen Berry, Abraham Nitzan, Peter Salamon

Physical review. A, General physics · 1977 · 180 citations · 8 references

Concepts

TL;DR

The step‑Carnot cycle resembles the reversible Carnot cycle but uses finite‑step pressure variations. The paper develops a method to bound work and heat in finite‑time processes and seeks to maximize step‑Carnot cycle effectiveness, efficiency, optimal period under finite heat conductance, and maximum power. The authors formulate a variational framework, solve model problems based on the step‑Carnot cycle, and analyze finite‑step equilibrium cycles to optimize effectiveness, efficiency, period, and power under finite heat conductance.

Abstract

The object of this paper is the beginning of a formulation of a method to find bounds to process functions, such as work and heat, for processes occurring in finite time. A general variational statement of the problem is given. Then model problems are solved, all but one of which are based on the "step-Carnot" cycle. This is similar to the reversible Carnot cycle but with the external pressure varying in finite steps. Such a system only needs to go through a finite number of equilibrium states during its cycle. The problems are the maximization of effectiveness of the step-Carnot cycle, the maximization of efficiency of the same cycle, the determination of optimal period for a step-Carnot cycle whose contact with the external reservoirs has finite heat conductance, and the determination of the maximum power and the rate at which maximum power is obtained, for a continuous Carnot cycle with finite heat conductance between system and thermostats.

References

8