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Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State

Observations of the surface domain structure (Kerr-effect), optical metallography, scanning electron microscopy (SEM-SE), and electron microprobe analysis (EPMA-SEM), measurements of major and minor magnetic hysteretic loops were used to study pseudo-single-crystal samples of (Sm,Zr)(Co,Cu,Fe)(z) al...

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Autores principales: Dormidontov, Andrey G., Kolchugina, Natalia B., Dormidontov, Nikolay A., Zheleznyi, Mark V., Bakulina, Anna S., Prokofev, Pavel A., Andreenko, Aleksandr S., Milov, Yury V., Sysoev, Nikolay N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8704425/
https://www.ncbi.nlm.nih.gov/pubmed/34947355
http://dx.doi.org/10.3390/ma14247762
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author Dormidontov, Andrey G.
Kolchugina, Natalia B.
Dormidontov, Nikolay A.
Zheleznyi, Mark V.
Bakulina, Anna S.
Prokofev, Pavel A.
Andreenko, Aleksandr S.
Milov, Yury V.
Sysoev, Nikolay N.
author_facet Dormidontov, Andrey G.
Kolchugina, Natalia B.
Dormidontov, Nikolay A.
Zheleznyi, Mark V.
Bakulina, Anna S.
Prokofev, Pavel A.
Andreenko, Aleksandr S.
Milov, Yury V.
Sysoev, Nikolay N.
author_sort Dormidontov, Andrey G.
collection PubMed
description Observations of the surface domain structure (Kerr-effect), optical metallography, scanning electron microscopy (SEM-SE), and electron microprobe analysis (EPMA-SEM), measurements of major and minor magnetic hysteretic loops were used to study pseudo-single-crystal samples of (Sm,Zr)(Co,Cu,Fe)(z) alloys subjected to heat treatments to the high-coercivity state, which are used in fabricating sintered permanent magnets. Correlations between the chemical composition, hysteretic properties, structural components, domain structure, and phase state were determined for the concentration ranges that ensure wide variations of 4f-/4d-/3d-element ratio in the studied samples. The phase state formed by collinear and coherent phase components determines the high coercive force and ultimate magnetic hysteresis loops of the pseudo-single crystals. It was found that the 1:5 phase with the hexagonal structure (P6/mmm) is the matrix of the alloys for (Sm,Zr)(Co,Cu,Fe)(z) permanent magnets; the matrix undergoes phase transformations in the course of all heat treatments for the high-coercivity state. The heterogeneity observed with optical magnifications, namely, the observation of main structural components A and B, is due to the alternation, within the common matrix, of regions with modulated quasi-spherical precipitates and regions with hexagonal bipyramids (cellular phase) although, traditionally, many investigators consider the cellular phase as the matrix. It is shown that the relationship of volume fractions of structural components A and B that account for more than 0.9 volume fraction of the total, which is due to the integral chemical composition of the alloys, determines the main hysteretic performances of the samples. The Zr-rich phases, such as 5:19, 2:7, and 6:23, and a structural component with the variable stoichiometry (Sm(Co,Cu,Fe)(3.5–5)) that is almost free of Zr and contains up to 33 at% Cu, were found only within structural component A in quantities sufficient for EPMA analysis.
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spelling pubmed-87044252021-12-25 Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State Dormidontov, Andrey G. Kolchugina, Natalia B. Dormidontov, Nikolay A. Zheleznyi, Mark V. Bakulina, Anna S. Prokofev, Pavel A. Andreenko, Aleksandr S. Milov, Yury V. Sysoev, Nikolay N. Materials (Basel) Article Observations of the surface domain structure (Kerr-effect), optical metallography, scanning electron microscopy (SEM-SE), and electron microprobe analysis (EPMA-SEM), measurements of major and minor magnetic hysteretic loops were used to study pseudo-single-crystal samples of (Sm,Zr)(Co,Cu,Fe)(z) alloys subjected to heat treatments to the high-coercivity state, which are used in fabricating sintered permanent magnets. Correlations between the chemical composition, hysteretic properties, structural components, domain structure, and phase state were determined for the concentration ranges that ensure wide variations of 4f-/4d-/3d-element ratio in the studied samples. The phase state formed by collinear and coherent phase components determines the high coercive force and ultimate magnetic hysteresis loops of the pseudo-single crystals. It was found that the 1:5 phase with the hexagonal structure (P6/mmm) is the matrix of the alloys for (Sm,Zr)(Co,Cu,Fe)(z) permanent magnets; the matrix undergoes phase transformations in the course of all heat treatments for the high-coercivity state. The heterogeneity observed with optical magnifications, namely, the observation of main structural components A and B, is due to the alternation, within the common matrix, of regions with modulated quasi-spherical precipitates and regions with hexagonal bipyramids (cellular phase) although, traditionally, many investigators consider the cellular phase as the matrix. It is shown that the relationship of volume fractions of structural components A and B that account for more than 0.9 volume fraction of the total, which is due to the integral chemical composition of the alloys, determines the main hysteretic performances of the samples. The Zr-rich phases, such as 5:19, 2:7, and 6:23, and a structural component with the variable stoichiometry (Sm(Co,Cu,Fe)(3.5–5)) that is almost free of Zr and contains up to 33 at% Cu, were found only within structural component A in quantities sufficient for EPMA analysis. MDPI 2021-12-15 /pmc/articles/PMC8704425/ /pubmed/34947355 http://dx.doi.org/10.3390/ma14247762 Text en © 2021 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
Dormidontov, Andrey G.
Kolchugina, Natalia B.
Dormidontov, Nikolay A.
Zheleznyi, Mark V.
Bakulina, Anna S.
Prokofev, Pavel A.
Andreenko, Aleksandr S.
Milov, Yury V.
Sysoev, Nikolay N.
Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title_full Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title_fullStr Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title_full_unstemmed Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title_short Structure of Alloys for (Sm,Zr)(Co,Cu,Fe)(z) Permanent Magnets: III. Matrix and Phases of the High-Coercivity State
title_sort structure of alloys for (sm,zr)(co,cu,fe)(z) permanent magnets: iii. matrix and phases of the high-coercivity state
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8704425/
https://www.ncbi.nlm.nih.gov/pubmed/34947355
http://dx.doi.org/10.3390/ma14247762
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