The role of Zr and B in room temperature magnetic entropy change of FeZrB amorphous alloys

2009 ◽  
Vol 95 (26) ◽  
pp. 262501 ◽  
Author(s):  
Yanyan Wang ◽  
Xiaofang Bi
2011 ◽  
Vol 84-85 ◽  
pp. 667-670
Author(s):  
Guo Qiu Xie

In this paper, we report on the structure, magnetic properties and magnetocaloric effect in NaZn13-type LaFe11.1Co0.8Si1.1Bxalloys close to room temperature. The stable NaZn13cubic structure phase (space group isFm-3c) can easily obtained by annealing at 1080 °C for 225 hours. The maximal values of magnetic entropy change for LaFe11.1Co0.8Si1.1Bx(x=0.2, 0.25) were found to be 5.3 and 5.9 J/kg K at Curie temperature for a magnetic field change in 0-1.5 T, respectively. The calculated refrigerant capacity for a field change in 0–1.5 T is about 147 and 107 J/kg K, for LaFe11.1Co0.8Si1.1B0.2and LaFe11.1Co0.8Si1.1B0.25respectively, which is as larger as those of Gd(99.3%) alloy


2002 ◽  
Vol 43 (1) ◽  
pp. 73-77 ◽  
Author(s):  
Hirofumi Wada ◽  
Kentaro Taniguchi ◽  
Yuji Tanabe

2007 ◽  
Vol 244 (12) ◽  
pp. 4570-4573 ◽  
Author(s):  
N. V. Dai ◽  
D. V. Son ◽  
S. C. Yu ◽  
L. V. Bau ◽  
L. V. Hong ◽  
...  

2018 ◽  
Vol 185 ◽  
pp. 05002
Author(s):  
Dan Nguyen ◽  
Ha Nguyen ◽  
An Nguyen ◽  
Yen Nguyen ◽  
Thanh Pham ◽  
...  

In this work, Pr2-xNdxFe17 (x = 0 - 2) ribbons with thickness of about 15 μm were prepared by melt-spinning method. The alloy ribbons were then annealed at different temperatures (900 - 1100°C) for various time (0.25 - 2 h). The formation of the (Pr,Nd)2Fe17 (2:17) crystalline phase in the alloys strongly depends on the Pr/Nd ratio and annealing conditions. Annealing time for the completed formation of the 2:17 phase in the rapidly quenched ribbons is greatly reduced in comparison with that of bulk alloys. Curie temperature, TC, of the alloys can be controlled in room temperature region by changing Pr/Nd ratio. Maximum magnetic entropy change (|ΔSm|max) and full width at haft the maximum peak (FWHM) of the magnetic entropy change of the alloys were respectively found to be larger than 1.5 J.kg−1K−1 and 40 K in room temperature region with magetic field change ΔH = 12 kOe.


RSC Advances ◽  
2019 ◽  
Vol 9 (41) ◽  
pp. 23598-23606 ◽  
Author(s):  
B. Arun ◽  
V. R. Akshay ◽  
M. Vasundhara

The effect of Sr-site deficiency on the structural, magnetic and magnetic entropy change of La0.67Sr0.33−yMnO3−δ (y = 0.18 and 0.27) compounds was investigated.


2013 ◽  
Vol 316-317 ◽  
pp. 996-1001 ◽  
Author(s):  
Zhe Li ◽  
Chao Jing ◽  
Jun Jun Wu ◽  
Ling Xian Wu ◽  
Jian Yin ◽  
...  

Effect of Co or Cu slightly introduced in Ni50Mn35In15on martensitic transformation and magnetocaloric effect was investigated. The small doping of Co can modify exchange interaction between Mn atoms, resulting in the ferromagnetic ordering of the parent phase and a large magnetization difference across the martensitic transformation. For Cu-doped sample, a large was obtained, and gives rise to a large magnetic entropy change of 58.4 J/kg K for 5 T near room temperature accompanying with smaller hysteresis losses. The study on the doping system may have significant impact on realization of room-temperature magnetic refrigeration.


2004 ◽  
Vol 13 (3) ◽  
pp. 393-396 ◽  
Author(s):  
Wang Fang ◽  
Chen Yuan-Fu ◽  
Wang Guang-Jun ◽  
Sun Ji-Rong ◽  
Shen Bao-Gen

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