Optimal Allocation of Heat Exchanger Area for Vapor-Compression Heat Pump Plants

Article Preview

Abstract:

In order to optimize coefficient of heat pump, the finite time thermodynamic optimization theory is applied in this paper. By introducing area ratio of the condenser and evaporator, the analytical expressions for the optimal allocation of heat exchanger area for the irreversible Carnot heat pump with variable-temperature heat reservoirs are derived. For illustration, a real vapor compression heat pump example is utilized. Empirical results show that the optimal values for real vapor-compression heat pump cycles are obtained when area ratio is equal to 0.916. The results can guide the evaluation of existing heat pump plants or influence design practice for future plants.The results can guide the evaluation of existing heat pump plants or influence design practice for future plants.

You might also be interested in these eBooks

Info:

Periodical:

Advanced Materials Research (Volumes 433-440)

Pages:

817-822

Citation:

Online since:

January 2012

Export:

Price:

Permissions CCC:

Permissions PLS:

Сopyright:

© 2012 Trans Tech Publications Ltd. All Rights Reserved

Share:

Citation:

[1] D B. Andresen, P. Salamon, R.S. Berry, Thermodynamics in finite time, Physics Today., vol. 9, p.62–70, (1984).

DOI: 10.1063/1.2916405

Google Scholar

[2] Chen L, Wu C, Sun F. Finite-time thermodynamic optimization or entropy-generation minimization of energy systems., Journal of Non-Equilibrium Thermodynamics, vol. 24 no. 4, 1999, p.327–59.

DOI: 10.1515/jnetdy.1999.020

Google Scholar

[3] Chen L, Sun F. Advances in finite-time thermodynamics: analysis and optimization., New York: Nova Science Publishers; (2004).

Google Scholar

[4] A. Durmayaz, O.S. Sogut, B. Sahin, H. Yavuz, Optimization of thermal systems based on finite-time thermodynamics and thermoeconomics, Progress in Energy and Combustion Science. vol. 30, 2004, p.175–217.

DOI: 10.1016/j.pecs.2003.10.003

Google Scholar

[5] C. Wu, Maximum obtainable specific cooling load of a refrigeration cycle, Energy Conversion and Management. vol. 36. 1995. p.7–10.

DOI: 10.1016/0196-8904(94)00035-x

Google Scholar

[6] Curzon FL, Ahlborn B. Efficiency of a Carnot engine at maximum power-output., Am J Phys . vol. 43. no. 1. 1975. p.22–24.

DOI: 10.1119/1.10023

Google Scholar

[7] Bejan A. Entropy-generation minimization: the new thermodynamics of finite-size devices and finite-time Processes,. J Appl Phys. vol. 79. no. 3. 1996. p.1191–218.

DOI: 10.1063/1.362674

Google Scholar

[8] Denton JC. Thermal cycles in classical thermodynamics and non-equilibrium thermodynamics in contrast with finite-time thermodynamics,. Energy Conversation Management. vol. 43. No. 13. 2002. p.1583–617.

DOI: 10.1016/s0196-8904(02)00074-2

Google Scholar

[9] Sun F, Chen W, Chen L, Wu C. Optimal performance of an endoreversible Carnot heat pump,. Energy Conversation Management. vol. 38. no. 14. 1997. p.1439–43.

DOI: 10.1016/s0196-8904(96)00013-1

Google Scholar

[10] Ni N, Chen L, Sun F, Wu C. Effect of heat-transfer law on the performance of a generalized irreversible Carnot heat-pump,. J Inst Energ . vol. 72. 1999. p.64–68.

DOI: 10.1238/physica.regular.064a00584

Google Scholar

[11] Chen L, Zhu X, Sun F. Exergy-based ecological optimization for a generalized irreversible Carnot heat-pump,. Energy Conversation Management. vol. 84. 2007. p.78–88.

DOI: 10.1016/j.apenergy.2006.04.003

Google Scholar