High-temperature materials and creep
Which statement about the γ' phase that provides the high-temperature strength of nickel-based superalloys is correct?
- AIt is a BCC (B2-type) ordered phase with a large lattice mismatch and incoherent interfaces with the matrix γ, so it precipitates as coarse particles at grain boundaries and in the grains that strongly pin dislocations
- BIt is Ni₃Al with the L1₂ ordered structure (an ordered phase based on FCC), with nearly the same lattice parameter as the matrix γ, and precipitates finely with coherent interfaces
- CIt is a carbide such as M₂₃C₆ that precipitates as a continuous film on grain boundaries; the more of it there is, the better grain boundary sliding is stopped and the higher both ductility and creep strength become
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Answer: B. It is Ni₃Al with the L1₂ ordered structure (an ordered phase based on FCC), with nearly the same lattice parameter as the matrix γ, and precipitates finely with coherent interfaces
The γ' phase is an L1₂ ordered phase of composition Ni₃(Al,Ti), in which Al occupies the corners and Ni the face centers of the FCC lattice. Its lattice parameter differs little from that of the matrix γ (an FCC Ni solid solution) (small misfit), so fine cuboidal particles precipitate with coherent interfaces, reaching 60 to 70% by volume in alloys for single-crystal blades. When a dislocation in γ enters γ', it disturbs the ordered arrangement and creates an antiphase boundary, so dislocations must travel in pairs, which gives a large resistance. γ' is stable up to high temperatures and also shows an anomalous temperature dependence in which the yield stress rises with temperature up to about 700 to 800 °C. Calling it BCC mistakes the crystal structure, and calling it a grain boundary carbide confuses it with another phase; a film-like carbide is actually a cause of brittleness.
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