4.7 Article

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

Journal

NANOMATERIALS
Volume 13, Issue 13, Pages -

Publisher

MDPI
DOI: 10.3390/nano13131899

Keywords

nanocrystalline cellular structure; permanent magnets; Sm2Co17; SmCo5

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This paper presents methods and approaches for producing high-temperature permanent magnets using Sm-Co-Fe-Cu-Zr alloys. The study shows that the content of Sm, Cu, and Fe significantly affects the coercivity value at high temperatures. Increasing the Sm content and decreasing the Fe content lead to an increase in coercivity at high temperatures. The optimal chemical composition for high-temperature permanent magnet application was determined by analyzing the dependence of temperature coefficients of the coercivity on the concentrations of various constituent elements.
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 & DEG;C. It is shown that the content of Sm, Cu, and Fe significantly affects the coercivity (H-c) 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 H-c value at room temperature, but significantly increase H-c at temperatures of about 500 & DEG;C. Increasing the Cu concentration enhances the H-c 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 Sm-2(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.

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