Performance optimization of low-dissipation thermal machines revisited
arXiv:1906.02453 · doi:10.1103/PhysRevE.100.052101
Abstract
We revisit the optimization of performance of finite-time Carnot machines satisfying the low-dissipation assumption. The standard procedure seeks to optimize an objective function, such as power output of the engine, over the durations of contacts between the working medium and the heat reservoirs. This procedure may lead to unwieldy equations at the optimum of some objective functions. We propose an alternate scheme in which the output or input work is first optimized for a given cycle time, followed by an optimization of another objective function over the cycle time. The optimal behavior is thus obtained in a much simplified manner, with closed-form expressions for figures of merit. The approach is demonstrated for various objective functions, both for engines as well as refrigerators.
6 pages, Revtex, discussion on Gouy-Stodola theorem added
References in corpus (6)
- Efficiency at maximum power: An analytically solvable model for stochastic heat engines
- Slow dynamics and thermodynamics of open quantum systems
- Coefficient of performance at maximum figure of merit and its bounds for low-dissipation Carnot-like refrigerators
- Low-dissipation Carnot-like heat engines at maximum efficient power
- Heat engines at optimal power: Low-dissipation versus endoreversible model
- Global linear-irreversible principle for optimization in finite-time thermodynamics