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Evolution of the Structural and Magnetic Properties of Bulk Fe(61)Co(10)B(20)W(1)Y(8−X)Pt(x) Alloys through the Partial Substitution of Pt for Y

This paper presents the results of an investigation into rapidly quenched Fe-based alloys with the chemical formula: Fe(61)Co(10)B(20)W(1)Y(8−x)Pt(x) (where x = 3, 4, 5). In these alloys, a small quantity of Pt was added, and the Y content was reduced concurrently. Samples of the aforementioned allo...

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Detalles Bibliográficos
Autores principales: Pietrusiewicz, Pawel, Nabiałek, Marcin, Jeż, Bartłomiej
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7663181/
https://www.ncbi.nlm.nih.gov/pubmed/33158199
http://dx.doi.org/10.3390/ma13214962
Descripción
Sumario:This paper presents the results of an investigation into rapidly quenched Fe-based alloys with the chemical formula: Fe(61)Co(10)B(20)W(1)Y(8−x)Pt(x) (where x = 3, 4, 5). In these alloys, a small quantity of Pt was added, and the Y content was reduced concurrently. Samples of the aforementioned alloys were injection-cast in the form of plates with the dimensions: 0.5 mm × 10 mm × 10 mm. The resulting structure was examined using X-ray diffractometry (XRD), Mössbauer spectroscopy and scanning electron microscopy (SEM). The results of the structural research reveal that, with a small addition of Pt, areas rich in Pt and Y are created—in which Fe-Pt and Pt-Y compounds, with different crystallographic systems, are formed. It has also been shown that an increase in Pt content, at the expense of Y, contributed to the formation of fewer crystalline phases, i.e., it allowed a material with a more homogeneous structure to be obtained. Magnetic properties of the Fe(61)Co(10)B(20)W(1)Y(8−x)Pt(x) (where x = 3, 4, 5) alloy samples were tested using a vibrating sample magnetometer (VSM). The magnetic properties of the investigated materials revealed that the saturation magnetisation increased with increasing Pt content, at the expense of Y. This effect is due to the occurrence of different proportions of crystalline magnetic phases within the volume of each alloy.