TY - JOUR
T1 - Thermodynamics in finite time. I. The step-Carnot cycle
AU - Andresen, Bjarne
AU - Berry, R. Stephen
AU - Nitzan, Abraham
AU - Salamon, Peter
N1 - Funding Information:
Partially supported by a travel grant from the Danish Science Foundation.
PY - 1977
Y1 - 1977
N2 - 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.
AB - 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.
UR - http://www.scopus.com/inward/record.url?scp=0001007735&partnerID=8YFLogxK
U2 - 10.1103/PhysRevA.15.2086
DO - 10.1103/PhysRevA.15.2086
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AN - SCOPUS:0001007735
SN - 1050-2947
VL - 15
SP - 2086
EP - 2093
JO - Physical Review A
JF - Physical Review A
IS - 5
ER -