Abstract
A systematic study of nickel-rich quinary alloys of the Ni-Fe-Cr-Ti-Al system has been made, confining attention to the 750° and 1000°C isothermals of the pseudo-quaternary section Ni3Cr-Ni3Fe-Ni3Ti-Ni3Al. Only three phases are involved, the nickel-rich face-centered-cubic primary γ-solid solution, the ordered face-centered-cubic Berthollide γ′-phase based on Ni3Al, and the hexagonal-close-packed Daltonide, η-Ni3Ti. The ternary face, Ni3Fe-Ni3Al-Ni3Ti, of the pseudo-quaternary tetrahedron is very similar to the ternary face Ni3Cr-Ni3Al-Ni3Ti because of iron replacing chromium atom for atom in the two face-centered-cubic phases, γ and γ′. The extent of the γ-solid solution increases considerably as the temperature is raised, while γ′ and η remain substantially unchanged. The tie-lines linking the γ and γ′-phases radiate uniformly across the γ + γ′ two-phase field of the pseudo-quaternary tetrahedron. Alloys situated near the Ni3Fe corner of the tetrahedron are strongly ferromagnetic. The boundary separating the magnetic from the nonmagnetic γ-phase alloys at room temperature is defined by a plane lying parallel to the Ni3Cr-Ni3Ti-Ni3Al face of the system and containing chromium and iron in the atomic ratio 60:40.
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References
A. Taylor: AIME Trans., 1956, vol. 206, p. 959; Journal of Metals, October 1956.
A. J. Bradley and A. Taylor: Proceedings Royal Soc., 1938, vol. 166A, p. 353.
A. J. Bradley: Journal Iron and Steel Inst., 1949, vol. 163, p. 19; 1951, vol. 168, p. 233.
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TP 4374E. Manuscript, Jan. 5, 1956. Cleveland Meeting, October 1956.
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Taylor, A. Constitution of nickel-rich quinary alloys in the system Ni-Fe-Cr-Ti-Al. JOM 9, 72–75 (1957). https://doi.org/10.1007/BF03398456
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DOI: https://doi.org/10.1007/BF03398456