Phase diagram of the Cu-Ni3Al pseudo-binary system
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作者:
Semboshi, Satoshi
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Tohoku Univ, Inst Mat Res, Katahira 2-1-1,Aoba Ku, Sendai, Miyagi 9808577, Japan
Osaka Prefecture Univ, Dept Mat Sci, Gakuen Cho 1-1,Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Inst Mat Res, Katahira 2-1-1,Aoba Ku, Sendai, Miyagi 9808577, Japan
Semboshi, Satoshi
[1
,2
]
Anno, Toshiki
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机构:
Osaka Prefecture Univ, Dept Mat Sci, Gakuen Cho 1-1,Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Inst Mat Res, Katahira 2-1-1,Aoba Ku, Sendai, Miyagi 9808577, Japan
Anno, Toshiki
[2
]
Kaneno, Yasuyuki
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Osaka Prefecture Univ, Dept Mat Sci, Gakuen Cho 1-1,Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Inst Mat Res, Katahira 2-1-1,Aoba Ku, Sendai, Miyagi 9808577, Japan
Kaneno, Yasuyuki
[2
]
机构:
[1] Tohoku Univ, Inst Mat Res, Katahira 2-1-1,Aoba Ku, Sendai, Miyagi 9808577, Japan
[2] Osaka Prefecture Univ, Dept Mat Sci, Gakuen Cho 1-1,Naka Ku, Sakai, Osaka 5998531, Japan
Cu-Ni-Al alloys with a Ni to Al ratio of approximately 3.0 are of particular interest for the development of electrically conductive products; thus, investigating their phase behavior is essential for achieving specific properties in these materials. In this study, the phase diagram of the Cu-Ni3Al pseudo-binary system was experimentally determined using cast and fully heat-treated Cu-Ni3Al alloys with a wide range of compositions, via microstructural observation and different quantitative analyses. The Cu-Ni3Al system undergoes a eutectic reaction Liquid ? alpha-Cu solid solution (Cu-ss) with an FCC structure +gamma '-Ni3Al with an ordered FCC L1(2 )structure. As the combined Ni and Al (Ni3Al) content increased, the microstructure transitioned from a single alpha-Cuss phase to two eutectic phases (alpha-Cuss and gamma '-Ni3Al), to a primary gamma '-Ni3Al phase and two eutectic phases, and to a single gamma '-Ni3Al phase. The solidus and liquidus temperatures increased with the (Ni+Al) content. The solid solubility of (Ni+Al) in the alpha-Cuss phase (C(Ni+Al)) could be described by an Arrhenius-type equation (ln C(Ni+Al) = 5.50 - 2637/T), indicating a significant temperature dependence. In contrast, the solubility of Cu in the gamma '-Ni3Al phase did not significantly decrease with the temperature. The phase diagram of the Cu-Ni3Al system was constructed from these results. The phase diagram will be useful in the development of Cu-Ni-Al alloys with exceptional strength and electrical conductivity. (C) 2022 Elsevier B.V. All rights reserved.
机构:
Tohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan
Osaka Prefecture Univ, Dept Mat Sci, Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan
Semboshi, Satoshi
Tsuda, Hiroyuki
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Osaka Prefecture Univ, Dept Mat Sci, Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan
Tsuda, Hiroyuki
Kaneno, Yasuyuki
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机构:
Osaka Prefecture Univ, Dept Mat Sci, Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan
Kaneno, Yasuyuki
Iwase, Akihiro
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Osaka Prefecture Univ, Dept Mat Sci, Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan
Iwase, Akihiro
Takasugi, Takayuki
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机构:
Osaka Prefecture Univ, Dept Mat Sci, Naka Ku, Sakai, Osaka 5998531, JapanTohoku Univ, Kansai Ctr, Inst Mat Res, Naka Ku, Sakai, Osaka 5998531, Japan