An absorption system, reduced to the equivalent combined system of three-heat-source heat pump, is optimized with economical criteria. The multiparameter thermodynamic function η combines the COP and rate of pumping, and determines that optimum. Values of μ = 0, μ = 1, and μ > 1 define three different cases of application for different markets.
Issue Section:
Technical Brief
1.
Chen
J.
Yan
Z.
1988
, “Equivalent Combined of Three-Heat-Source Heat Pumps
,” Journal of Chemistry and Physics
, Vol. 90
(9
), pp. 4951
–4955
.2.
Curzon
Ahlborn
1975
, “Efficiency of a Carnot Engine at Maximum Power Output
,” American Journal of Physics
, Vol. 43
, pp. 22
–24
.3.
Huang, F. F., 1976, Engineering Thermodynamics, Macmillan, New York, NY.
4.
Ku¨mmell
R.
1989
, “Energy as Factor of Production and Entropy as a Pollution Indicator in Macroeconomic Modelling
,” Ecological Economics
, Vol. 1
, pp. 161
–180
.5.
Ondrechen
M. J.
Rubin
M. H.
Band
Y. B.
1983
, “The Generalized Cannot Cycle: A Working Fluid Operating in Finite Time Between Finite Heat Sources and Sinks
,” Journal of Chemistry and Physics
, Vol. 78
(7
), pp. 4721
–4727
.6.
Rubin
M. H.
1979
, “Optimal Configuration of a Class of Irreversible Heat Engines
,” Physics Review A
, Vol. 19
, pp. 1272
–1276
.7.
Salomon
P.
Nitzan
A.
1981
, “Finite Time Optimizations of a Newton’s Law Cannot Cycle
,” Journal of Chemistry and Physics
, Vol. 74
(6
), pp. 3546
–3560
.
This content is only available via PDF.
Copyright © 1996
by The American Society of Mechanical Engineers
You do not currently have access to this content.