Achieving Carnot efficiency in a finite-power Brownian Carnot cycle with arbitrary temperature difference
arXiv:2112.02276 · doi:10.1103/PhysRevE.105.034102
Abstract
Achieving the Carnot efficiency at finite power is a challenging problem in heat engines due to the trade-off relation between efficiency and power that holds for general heat engines. It is pointed out that the Carnot efficiency at finite power may be achievable in the vanishing limit of the relaxation times of a system without breaking the trade-off relation. However, any explicit model of heat engines that realizes this scenario for arbitrary temperature difference has not been proposed. Here, we investigate an underdamped Brownian Carnot cycle where the finite-time adiabatic processes connecting the isothermal processes are tactically adopted. We show that in the vanishing limit of the relaxation times in the above cycle, the compatibility of the Carnot efficiency and finite power is achievable for arbitrary temperature difference. This is theoretically explained based on the trade-off relation derived for our cycle, which is also confirmed by numerical simulations.
16pages, 8 figures
References in corpus (8)
- Efficiency at maximum power: An analytically solvable model for stochastic heat engines
- Strong bounds on Onsager coefficients and efficiency for three terminal thermoelectric transport in a magnetic field
- Adiabatic processes realized with a trapped Brownian particle
- Chiral thermoelectrics with quantum Hall edge states
- Efficiency of three-terminal thermoelectric transport under broken-time reversal symmetry
- Efficiency bounds on thermoelectric transport in magnetic fields: The role of inelastic processes
- Quantum Nernst engines
- Compatibility of Carnot efficiency with finite power in an underdamped Brownian Carnot cycle in small temperature-difference regime
Cited by in corpus (6)
- Geometric characterization for cyclic heat engines far from equilibrium
- Maximum Power of Coupled-Qubit Otto Engines
- Decomposition of metric tensor in thermodynamic geometry in terms of relaxation timescales
- Geometric Bounds on the Power of Adiabatic Thermal Machines
- Lower Bound of Entropy Production in an Underdamped Langevin System with Normal Distributions
- False Onsager relations