Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity

Author:

Golovnia O. A.12ORCID,Popov A. G.1,Mushnikov N. V.1ORCID,Protasov A. V.12ORCID,Pradeep K. G.3,Ogurtsov A. V.4,Taranov D. V.4,Tishin A. M.5ORCID

Affiliation:

1. M.N. Mikheev Institute of Metal Physics of Ural Branch of RAS, 620108 Ekaterinburg, Sverdlovsk Region, Russia

2. Institute of Natural Sciences and Mathematics, Ural Federal University, 620002 Ekaterinburg, Sverdlovsk Region, Russia

3. Correlative Microscopy Lab, Department of Metallurgical and Materials Engineering, Indian Institute of Technology Madras, Chennai 600036, India

4. LLC “POZ-Progress”, 624092 Verkhnyaya Pyshma, Sverdlovsk Region, Russia

5. Faculty of Physics, M.V.Lomonosov Moscow State University, 119991 Moscow, Russia

Abstract

This paper presents methods and approaches that can be used for production of Sm-Co-Fe-Cu-Zr permanent magnets with working temperatures of up to 550 °C. It is shown that the content of Sm, Cu, and Fe significantly affects the coercivity (Hc) value at high operating temperatures. A decrease in the content of Fe, which replaces Co, and an increase in the content of Sm in Sm-Co-Fe-Cu-Zr alloys lead to a decrease in Hc value at room temperature, but significantly increase Hc at temperatures of about 500 °C. Increasing the Cu concentration enhances the Hc values at all operating temperatures. From analysis of the dependence of temperature coefficients of the coercivity on the concentrations of various constituent elements in this alloy, the optimum chemical composition that qualifies for high-temperature permanent magnet (HTPM) application were determined. 3D atom probe tomography analysis shows that the nanostructure of the HTPM is characterized by the formation of Sm2(Co,Fe)17 (2:17) cells relatively smaller in size along with the slightly thickened Sm(Co,Cu)5 (1:5) boundary phase compared to those of the high-energy permanent magnet compositions. An inhomogeneous distribution of Cu was also noticed in the 1:5 phase. At the boundary between 1:5 and 2:17 phases, an interface with lowered anisotropy constants has developed, which could be the reason for the observed high coercivity values.

Funder

state assignment of the Ministry of Education and Science of Russia

Development Program of the Ural Federal University

Publisher

MDPI AG

Subject

General Materials Science,General Chemical Engineering

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