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

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 (H(c)) value at high operating temperatures. A decrease in the...

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Autores principales: Golovnia, O. A., Popov, A. G., Mushnikov, N. V., Protasov, A. V., Pradeep, K. G., Ogurtsov, A. V., Taranov, D. V., Tishin, A. M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10343306/
https://www.ncbi.nlm.nih.gov/pubmed/37446415
http://dx.doi.org/10.3390/nano13131899
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author Golovnia, O. A.
Popov, A. G.
Mushnikov, N. V.
Protasov, A. V.
Pradeep, K. G.
Ogurtsov, A. V.
Taranov, D. V.
Tishin, A. M.
author_facet Golovnia, O. A.
Popov, A. G.
Mushnikov, N. V.
Protasov, A. V.
Pradeep, K. G.
Ogurtsov, A. V.
Taranov, D. V.
Tishin, A. M.
author_sort Golovnia, O. A.
collection PubMed
description 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 (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 °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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spelling pubmed-103433062023-07-14 Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity Golovnia, O. A. Popov, A. G. Mushnikov, N. V. Protasov, A. V. Pradeep, K. G. Ogurtsov, A. V. Taranov, D. V. Tishin, A. M. Nanomaterials (Basel) Article 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 (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 °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. MDPI 2023-06-21 /pmc/articles/PMC10343306/ /pubmed/37446415 http://dx.doi.org/10.3390/nano13131899 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Golovnia, O. A.
Popov, A. G.
Mushnikov, N. V.
Protasov, A. V.
Pradeep, K. G.
Ogurtsov, A. V.
Taranov, D. V.
Tishin, A. M.
Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title_full Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title_fullStr Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title_full_unstemmed Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title_short Hard Magnetic Properties and the Features of Nanostructure of High-Temperature Sm-Co-Fe-Cu-Zr Magnet with Abnormal Temperature Dependence of Coercivity
title_sort hard magnetic properties and the features of nanostructure of high-temperature sm-co-fe-cu-zr magnet with abnormal temperature dependence of coercivity
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10343306/
https://www.ncbi.nlm.nih.gov/pubmed/37446415
http://dx.doi.org/10.3390/nano13131899
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