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Magnetic Refrigeration (at room temperature)

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Presentation on theme: "Magnetic Refrigeration (at room temperature)"— Presentation transcript:

1 Magnetic Refrigeration (at room temperature)
Behzad Monfared

2 Agenda Introduction Computer simulation Prototype
Solid-state magnetic refrigeration Future work

3 Magnetocaloric effect
Temperature increase in presence of magnetic field (magnetocaloric effect) Example: Gd (rare-earth metal)

4 Working principle

5 Thermodynamic cycle Resembles Brayton cycle Limited span Regeneration

6 Regeneration

7 Active regeneration

8 Porous regenerator Packed bed Parallel plates
(Tusek et al. 2013)

9 A built prototype (not ours)
Cold heat exchanger Bahl et al., 2012, Thermag V Conf., Grenoble

10 Technical Aspects of a Magnetic Refrigerator
Hydraulics Mechanics Material science Magnetism Thermodynamics Heat transfer - Bed of MC material - Valves and connections - Heat exchangers - Pumping power - Bed of MC material - Heat losses - Heat exchangers - Power transmission losses - Mechanisms - Magnetic and non-magnetic properties - Mechanics of Material - Hysteresis, Volume change, etc. - Magnetocaloric effect - Bed of MC material - Heat exchangers - Energy balance and performance evaluation - Design of the magnet assembly - Field variations (spatial and temporal) - Magnetic forces - Magnetization of the MC materials - Eddy currents

11 Advantages No leakage of refrigerants
Magnetization/demagnetization is reversible unlike compression/expansion Potential for higher efficiency the most promising alternative to vapor-compression technology (compared to Thermoelectric, Stirling, Electrocaloric, etc.) (Qian et al. 2016)

12 Agenda Introduction Computer simulation Prototype
Solid-state magnetic refrigeration Future work

13 Mathematical model Solid
𝑘 𝑒𝑠 𝜕 2 𝑇 𝑠 𝜕 𝑥 2 + ℎ 𝑠𝑓 𝑎 𝑇 𝑓 − 𝑇 𝑠 − 1−𝜀 𝜌 𝑠 𝑇 𝑠 𝜕𝑠 𝜕𝐵 𝜕𝐵 𝜕𝑡 =(1−𝜀) 𝜌 𝑠 𝑐 𝑝,𝑠 𝜕 𝑇 𝑠 𝜕𝑡 Fluid 𝑘 𝑒𝑓 𝜕 2 𝑇 𝑓 𝜕 𝑥 2 − 𝑉 𝐷 𝑐 𝑝,𝑓 𝜕 𝑇 𝑓 𝜕𝑥 − ℎ 𝑠𝑓 𝑎 𝑇 𝑓 − 𝑇 𝑠 + 𝑑𝑃 𝑑𝑥 𝑉 𝐷 =𝜀 𝜌 𝑓 𝑐 𝑝,𝑓 𝜕 𝑇 𝑓 𝜕𝑡 Monfared and Palm "Optimization of layered regenerator of a magnetic refrigeration device." International Journal of Refrigeration 57: doi:

14 Agenda Introduction Computer simulation Prototype
Solid-state magnetic refrigeration Future work

15 Design specifications
200 W cooling capacity over 40 K temperature span Estimated 1.6 COP Magnetic field indicates cost, weight, and size Comparison: (Jacobs et al. 2014) 2000 W over 12 K temperature span with 1.44 T field * defined differently cooling capacity [W] (zero span) temperature span* [K] (zero load) magnetic field [T] (Zimm et al. 2006) 50 25 1.5 (Okamura et al. 2007) 560 8 1.1 (Vasile and Müller 2006) 360 14 2.4 (Yao et al. 2006) 51 42 (Lozano 2014) 625 1.24

16 Regenerators

17 Magnetic circuit

18 Measured results (1/6 of the capacity)

19 Materials: the main problem
Pulverization (low mechanical strength) Corrosion Non-uniform size of particles Low quality of delivery Resulting in excessive pressure drop, low performance, clogging, etc.

20 Agenda Introduction Computer simulation Prototype
Solid-state magnetic refrigeration Future work

21 Another work in parallel
Low cycle frequency of the conventional magnetic refrigeration systems described Small cooling capacity per kg of magnetocaloric material Large magnets ( 𝑚 𝑚𝑎𝑔 𝑚 𝑀𝐶𝑀 does not increase linearly) Expensive and bulky Solid-state magnetic refrigeration

22 Solid-state magnetic refrigeration
Enhanced conduction in one direction

23 Agenda Introduction Computer simulation Prototype
Solid-state magnetic refrigeration Future work

24 Future work Solving the remaining problems of the prototype
Running systematic experiments to study the effect of different parameters Adjusting the software model using the experimental data Simulating solid-state magnetic refrigeration systems

25 Thank you


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