Abstract
In this paper, a thermodynamic model for predicting the performance of active magnetic refrigerator (AMR) is developed using energy and exergy analyses. Through this model, the cooling power, total power consumption, as well as the coefficient of performance (COP), exergy efficiency and exergy destruction rates of an AMR are determined. The effects of increasing mass flow rate on the COP, exergy efficiency and exergy destruction rates of the system are investigated. The results are presented to show that when mass flow rate increases, the COP and exergy efficiency curves reach their maximum values and then slightly decreases with increasing mass flow rate. The rate of exergy destruction increases with increasing mass flow rate due to the pump power requirements. The numerical results show that in order to reach optimal performance, mass flow rate must be adjusted carefully regarding to different operating conditions.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
References
Ganjehsarabi H, Dincer I, Gungor A (2013) Thermodynamic analysis and performance assessment of a cascade active magnetic regenerative refrigeration system. Int J Air Cond Ref 21(3):1350016.1–1350016.10
Barclay JA, Steyert WA (1982) Active magnetic regenerator. US patent No. 4332135, 1982
Brown GV (1976) Magnetic heat pumping near temperature. J Appl Phys 47:3673–3680
Aprea C, Greco A, Maiorino A (2013) A dimensionless numerical analysis for the optimization of an active magnetic regenerative refrigerant cycle. Int J Energy Res 37:1475–1487
Aprea C, Greco A, Maiorino A (2011) A numerical analysis of an active magnetic regenerative cascade system. Int J Energy Res 35:177–188
Tagliafico G, Scarpa F, Tagliafico LA (2010) A dynamic 1-D model for a reciprocating active magnetic regenerator; influence of the main working parameters. Int J Refrig 33(2):286–293
Yu B, Liu M, Egolf PW, Kitanovski A (2010) A review of magnetic refrigerator and heat pump prototypes built before 2010. Int J Refrig 33(6):1029–1060
Arnold DS, Tura A, Ruebsaat-Trott A, Rowe A (2014) Design improvements of a permanent magnet active magnetic refrigerator. Int J Refrig 37:99–105
Lozano JA, Engelbrecht K, Bahl CRH, Nielsen KK, Eriksen D, Barbosa JR, Smith A, Prata AT, Pryds N, Olsen UL (2013) Performance analysis of a rotary active magnetic refrigerator. Appl Energy 111:669–680
Zimm C, Boeder A, Chell J, Sternberg A, Fujita A, Fujieda S, Fukamichi K (2006) Design and performance of a permanent-magnet rotary refrigerator. Int J Refrig 29:1302–1306
Okamura T, Yamada K, Hirano N, Nagaya S (2006) Performance of a room temperature rotary magnetic refrigerator. Int J Refrig 29:1327–1331
Hall JL, Reid CE, Spearing IG, Barclay JA (1996) Thermodynamic considerations for the design of active magnetic regenerative refrigerators. Adv Cryogenic Eng 41:1653–1663
Rosario L, Rahman M (2010) Analysis of a magnetic refrigerator. Appl Therm Eng 31:1082–1090
Rohsenow WM, Hartnett JP, Ganic ENI (1985) Handbook of heat transfer, vol 6. McGraw-Hill, New York, NY, pp 10–11
Kaviany M (1995) Principles of heat transfer in porous media. Springer, New York, NY
Ganjehsarabi H, Dincer I, Gungor A (2014) Exergoeconomic analysis of a cascade active magnetic regenerative refrigeration system. Progress in exergy, energy, and the environment. 69–80
Author information
Authors and Affiliations
Corresponding author
Editor information
Editors and Affiliations
Nomenclature
Nomenclature
- Ac:
-
Cross-sectional area m2
- asf :
-
Specific surface area m2/m3
- c:
-
Specific heat J kg K−1
- COP:
-
Coefficient of performance
- D:
-
Diameter of the regenerator section m
- dP :
-
Diameter of the particles μm
- \( \dot{\mathrm{E}}\mathrm{x} \) :
-
Exergy flow rate (W)
- h:
-
Convection coefficient (W m−2 K−1)
- H:
-
Magnetic field A m−1
- Hmax :
-
Maximum magnetic field A m−1
- k:
-
Thermal conductivity W m−1 K−1
- L:
-
Length of the regenerator m
- m:
-
Mass kg
- \( \dot{\mathrm{m}} \) :
-
Mass flow rate kg s−1
- M:
-
Magnetic intensity A m−1
- Nu:
-
Nusselt number
- Pr:
-
Prandtl number
- \( \dot{Q} \) :
-
Heat transfer rate, W
- Re:
-
Reynolds number dimensionless
- s:
-
Specific entropy (J kg−1 K−1)
- t:
-
Time coordinate s
- t1 :
-
Magnetization time step (s)
- t2 :
-
Isofield cooling time step (s)
- t3 :
-
Demagnetization time step (s)
- t4 :
-
Isofield heating time step (s)
- T:
-
Temperature K
- u:
-
Local velocity m/s
- V:
-
Volume L
- X:
-
Axial position m
- \( \dot{W} \) :
-
Work kJ s−1
- ΔP:
-
Pressure drop Pa
- ε :
-
Porosity of the regenerator bed
- μ 0 :
-
Permeability of free space (m kg s−2 A−2)
- ρ :
-
Density kg m−3
- η :
-
Efficiency (−)
- ad:
-
Adiabatic
- C:
-
Cooling
- D:
-
Demagnetization
- des:
-
Destruction
- ex:
-
Exergy
- f:
-
Fluid
- H:
-
Rejection
- M:
-
Magnetic
- P:
-
Pump
- s:
-
Solid
Rights and permissions
Copyright information
© 2014 Springer International Publishing Switzerland
About this chapter
Cite this chapter
Ganjehsarabi, H., Dincer, I., Gungor, A. (2014). Energy and Exergy Analyses of an Active Magnetic Refrigerator. In: Dincer, I., Midilli, A., Kucuk, H. (eds) Progress in Sustainable Energy Technologies Vol II. Springer, Cham. https://doi.org/10.1007/978-3-319-07977-6_1
Download citation
DOI: https://doi.org/10.1007/978-3-319-07977-6_1
Published:
Publisher Name: Springer, Cham
Print ISBN: 978-3-319-07976-9
Online ISBN: 978-3-319-07977-6
eBook Packages: EnergyEnergy (R0)