Effects of Sn and Gd on the (β1 + β3) stability field in the Cu-11%Al-10%Mn alloy

Effects of Sn and Gd additions on the (β 1  + β 3 ) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry, non-isothermal kinetics, and magnetization measurements as a function of the temperature. The microstructures were investigated using op...

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Published inJournal of thermal analysis and calorimetry Vol. 148; no. 6; pp. 2357 - 2366
Main Authors Souza, J. S., Silva, L. S., Bessa, C. V. X., Silva, R. A. G.
Format Journal Article
LanguageEnglish
Published Cham Springer International Publishing 01.03.2023
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Abstract Effects of Sn and Gd additions on the (β 1  + β 3 ) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry, non-isothermal kinetics, and magnetization measurements as a function of the temperature. The microstructures were investigated using optical microscopy and scanning electron microscopy coupled with energy-dispersive X-ray spectroscopy. The results showed that the β 3 Cu 2 AlMn + β 1 Cu 3 Al → β 3 Cu 2 AlMn reaction is strongly dependent on the heating and cooling rates. The Sn addition to the Cu-11%Al-10%Mn alloy stabilizes the ferromagnetic β 3 phase. In the Sn-containing alloy, the miscibility gap transition is followed by the martensitic transformation at about 560 K. Both Sn and Gd additions have extended the stability field of the ferromagnetic β 3 phase. Nonetheless, the formation of Cu 5 Gd precipitates slows the miscibility gap transition on heating, which may be associated with the reduction of the ferromagnetic phase amount at room temperature in the Cu11%Al10%Mn3%Gd alloy.
AbstractList Effects of Sn and Gd additions on the (β1 + β3) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry, non-isothermal kinetics, and magnetization measurements as a function of the temperature. The microstructures were investigated using optical microscopy and scanning electron microscopy coupled with energy-dispersive X-ray spectroscopy. The results showed that the β3Cu2AlMn+β1Cu3Al→β3Cu2AlMn reaction is strongly dependent on the heating and cooling rates. The Sn addition to the Cu-11%Al-10%Mn alloy stabilizes the ferromagnetic β3 phase. In the Sn-containing alloy, the miscibility gap transition is followed by the martensitic transformation at about 560 K. Both Sn and Gd additions have extended the stability field of the ferromagnetic β3 phase. Nonetheless, the formation of Cu5Gd precipitates slows the miscibility gap transition on heating, which may be associated with the reduction of the ferromagnetic phase amount at room temperature in the Cu11%Al10%Mn3%Gd alloy.
Effects of Sn and Gd additions on the (β 1  + β 3 ) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry, non-isothermal kinetics, and magnetization measurements as a function of the temperature. The microstructures were investigated using optical microscopy and scanning electron microscopy coupled with energy-dispersive X-ray spectroscopy. The results showed that the β 3 Cu 2 AlMn + β 1 Cu 3 Al → β 3 Cu 2 AlMn reaction is strongly dependent on the heating and cooling rates. The Sn addition to the Cu-11%Al-10%Mn alloy stabilizes the ferromagnetic β 3 phase. In the Sn-containing alloy, the miscibility gap transition is followed by the martensitic transformation at about 560 K. Both Sn and Gd additions have extended the stability field of the ferromagnetic β 3 phase. Nonetheless, the formation of Cu 5 Gd precipitates slows the miscibility gap transition on heating, which may be associated with the reduction of the ferromagnetic phase amount at room temperature in the Cu11%Al10%Mn3%Gd alloy.
Effects of Sn and Gd additions on the ([beta].sub.1 + [beta].sub.3) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry, non-isothermal kinetics, and magnetization measurements as a function of the temperature. The microstructures were investigated using optical microscopy and scanning electron microscopy coupled with energy-dispersive X-ray spectroscopy. The results showed that the [Formula omitted] reaction is strongly dependent on the heating and cooling rates. The Sn addition to the Cu-11%Al-10%Mn alloy stabilizes the ferromagnetic [beta].sub.3 phase. In the Sn-containing alloy, the miscibility gap transition is followed by the martensitic transformation at about 560 K. Both Sn and Gd additions have extended the stability field of the ferromagnetic [beta].sub.3 phase. Nonetheless, the formation of Cu.sub.5Gd precipitates slows the miscibility gap transition on heating, which may be associated with the reduction of the ferromagnetic phase amount at room temperature in the Cu11%Al10%Mn3%Gd alloy.
Audience Academic
Author Bessa, C. V. X.
Souza, J. S.
Silva, L. S.
Silva, R. A. G.
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Keywords Gd addition
Cu-Al-Mn alloys
Kinetics
Miscibility gap
Sn addition
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Snippet Effects of Sn and Gd additions on the (β 1  + β 3 ) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning...
Effects of Sn and Gd additions on the ([beta].sub.1 + [beta].sub.3) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential...
Effects of Sn and Gd additions on the (β1 + β3) field in the Cu-11%Al-10%Mn alloy were studied by in situ X-ray diffraction, differential scanning calorimetry,...
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SubjectTerms Alloying effects
Alloys
Aluminum
Analysis
Analytical Chemistry
Calorimetry
Chemistry
Chemistry and Materials Science
Cooling rate
Copper
Copper base alloys
Diffraction
Ferromagnetic phases
Ferromagnetism
Gadolinium
Heating
Inorganic Chemistry
Magnetization
Manganese base alloys
Martensitic transformations
Measurement Science and Instrumentation
Miscibility
Optical microscopy
Physical Chemistry
Polymer Sciences
Precipitates
Room temperature
Stability
Thermal properties
Tin
X-ray spectroscopy
X-rays
Title Effects of Sn and Gd on the (β1 + β3) stability field in the Cu-11%Al-10%Mn alloy
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