Effect of Cu substitution on structural and hard magnetic properties of rapidly solidified Zr 18 Co 82-x Cu x melt spun ribbons

2017 ◽  
Vol 699 ◽  
pp. 657-661 ◽  
Author(s):  
M.D. Imtyaz ◽  
N.V. Rama Rao ◽  
D. Aravindha Babu ◽  
B. Ramesh Chandra ◽  
S. Pandian
2012 ◽  
Vol 112 (8) ◽  
pp. 083901 ◽  
Author(s):  
Tetsuji Saito ◽  
Ryuji Nishimura

1985 ◽  
Vol 58 ◽  
Author(s):  
G.C. Hadjipanayis

ABSTRACTThe magnetic and structural properties of melt-spun Fe-R-B alloys are reviewed. The hard magnetic properties of these alloys are attributed to the presence of a highly anisotropic tetragonal phase Fe14R2B which in the case of ribbons occurs in very fine grains. The interachoot of domain walls with this fine microstructure leads to the observed high coercivities. The effects of partial substitution of iron, rare-earth and boron on the formation of Fe14R2B and on its magnetic properties are also discussed.


2020 ◽  
Vol 128 (15) ◽  
pp. 153901
Author(s):  
Kinjal Gandha ◽  
Xubo Liu ◽  
Wei Tang ◽  
I. C. Nlebedim

2002 ◽  
Vol 91 (11) ◽  
pp. 9267-9271 ◽  
Author(s):  
Z. G. Sun ◽  
W. Löser ◽  
J. Eckert ◽  
K.-H. Müller ◽  
L. Schultz

2018 ◽  
Vol 97 ◽  
pp. 89-94 ◽  
Author(s):  
Anil Aryal ◽  
Abdiel Quetz ◽  
C.F. Sánchez-Valdés ◽  
P.J. Ibarra-Gaytán ◽  
Sudip Pandey ◽  
...  

2018 ◽  
Vol 31 (11) ◽  
pp. 3705-3710 ◽  
Author(s):  
Chengfu Xu ◽  
Kanghua Chen ◽  
Zhengfei Gu ◽  
Guanghui Rao ◽  
Gang Cheng ◽  
...  

2021 ◽  
Vol 21 (4) ◽  
pp. 2552-2557
Author(s):  
Nguyen Hai Yen ◽  
Nguyen Hoang Ha ◽  
Pham Thi Thanh ◽  
Nguyen Huy Ngoc ◽  
Tran Dang Thanh ◽  
...  

In this work, we investigated magnetic properties and magnetocaloric effect in Fe90−xCoxZr7Cu1B2 (x = 0, 1, 2, 3 and 4) melt-spun ribbons. The ribbons were prepared by using a melt-spinning method with a tangential velocity of a copper wheel of 40 m·s-1. The obtained ribbons are almost amorphous. The alloys exhibit typical soft magnetic behavior with low coercivity at room temperature. A minor replacement of Fe by Co gives an increment in Curie temperature (TC) of the alloys to higher temperatures. The TC of the alloys increases from 242 to 342 K with an increase of x from 0 to 4. Maximum magnetic entropy change, ΔSm max, of the alloys, was found to be larger than 0.7 J·kg-1·K-1 in a magnetic field change ΔH of 12 kOe for all the concentrations of Co. High refrigerant capacitys (RC >100 J ·kg-1 with ΔH = 12 kOe) at room temperature region have been obtained for the alloys. The large magnetocaloric effect near room temperature suggests that the alloys can be considered as magnetic refrigerants in the range of 250–350 K.


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