Significant optimization of active thermomagnetic generator for low-grade waste heat recovery

被引:8
|
作者
Liu, Xianliang [1 ]
Zhang, Hu [1 ]
Chen, Haodong [1 ]
Ma, Zhihui [1 ]
Qiao, Kaiming [1 ]
Xie, Longlong [1 ]
Ou, Zhiqiang [2 ]
Wang, Jing [3 ,4 ,5 ]
Hu, Fengxia [3 ,4 ,6 ]
Shen, Baogen [3 ,4 ,7 ]
机构
[1] Univ Sci & Technol Beijing, Sch Mat Sci & Engn, Beijing 100083, Peoples R China
[2] Inner Mongolia Normal Univ, Inner Mongolia Key Lab Phys & Chem Funct Mat, Hohhot 010022, Peoples R China
[3] Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
[4] Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100049, Peoples R China
[5] Chinese Acad Sci, Fujian Innovat Acad, Fuzhou 350108, Fujian, Peoples R China
[6] Songshan Lake Mat Lab, Dongguan 523808, Guangdong, Peoples R China
[7] Chinese Acad Sci, Ningbo Inst Mat Technol & Engn, Ningbo 315201, Zhejiang, Peoples R China
基金
中国国家自然科学基金; 中国博士后科学基金;
关键词
Thermomagnetic generator; Waste heat recovery; Thermomagnetic effect; Energy conversion; THERMAL TRANSPORT-PROPERTIES; THERMOELECTRIC GENERATORS; CONVERSION; FEASIBILITY; PERFORMANCE; CO;
D O I
10.1016/j.applthermaleng.2022.119827
中图分类号
O414.1 [热力学];
学科分类号
摘要
Recently, thermomagnetic generator (TMG) based on the thermomagnetic effect is becoming a promising technology for low-grade waste heat recovery. However, poor performance still hinders the application of this novel technology. The performance of TMG is significantly affected by the key device parameters and material properties. Unfortunately, there is a lack of systematic research in this regard. In present work, for the first time, we systematically study the effects of different key device and material parameters on the TMG performance through a combination of experiment and finite element simulation. It demonstrates that the TMG performance is influenced largely by both device and material parameters, especially the cabin size and specific heat capacity. Furthermore, the key device parameters are optimized, i.e., the sample cabin size is shortened from 145 mm to 20 mm, the system temperature range is expanded from 288 -353 K to 276 -361 K, and the cycle period is reduced from 60 s to 10 s. In comparison with the non-optimized experimental peak I of 28.8 mu A, the simulated peak I increases largely to 136.1 mu A after the optimization. In addition, more I peaks are obtained by shortening the cycle period. The maximum power density Pd and average Pd are 3.6 mW/m3 K and 0.4 mW/m3 K, respectively, which are one order of magnitude higher than the values before optimization (0.16 mW/m3 K and 0.01 mW/m3 K), and even three orders of magnitude higher than those of other reported TMGs.
引用
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页数:12
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