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A1→D022Transformation and Multi-Variant Structure of Ni3V

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ABSTRACTThe formation mechanism and morphology of the tetragonal compound Ni3V (D022) quenched from the disordered fcc (A1) state have been examined by TEM using a Ni-25at%V. The alloy is fully transformed to D022in the quenched state. The resulting microstructure exhibits a fine brick-like “multi-variant structure (MVS)” consisting of one major and two minor variants withcaxes perpendicular each other, having coherent interfaces of {102)D022and {100)D022. The major variant particles with a quadrangular-prism shape are alternately arrayed with two minor variants, one parallel to {102)D022and the other {100)D022, respectively. The thermal APDs are formed in the all variants, but the average size within the major is larger than that in the minors. The c/a ratio of the D022in the MVS is 2.006, much smaller than the value (2.04) in equilibrium state. From all these facts, the transformation of A1→D022is assumed to proceed through a selective nucleation and growth of tetragonal A6 phase, followed by ordering to D022. The formation of the tetragonal phase produces an anisotropic strain field due to the contraction and expansion of theaandcaxes against the cubic matrix. The strain field makes {102)D022and {100)D022with the invariant lines become habit, and also drives the selective nucleation and growth of minor variants to minimize the elastic strain energy, thereby leading to the multi-variant structure.
Title: A1→D022Transformation and Multi-Variant Structure of Ni3V
Description:
ABSTRACTThe formation mechanism and morphology of the tetragonal compound Ni3V (D022) quenched from the disordered fcc (A1) state have been examined by TEM using a Ni-25at%V.
The alloy is fully transformed to D022in the quenched state.
The resulting microstructure exhibits a fine brick-like “multi-variant structure (MVS)” consisting of one major and two minor variants withcaxes perpendicular each other, having coherent interfaces of {102)D022and {100)D022.
The major variant particles with a quadrangular-prism shape are alternately arrayed with two minor variants, one parallel to {102)D022and the other {100)D022, respectively.
The thermal APDs are formed in the all variants, but the average size within the major is larger than that in the minors.
The c/a ratio of the D022in the MVS is 2.
006, much smaller than the value (2.
04) in equilibrium state.
From all these facts, the transformation of A1→D022is assumed to proceed through a selective nucleation and growth of tetragonal A6 phase, followed by ordering to D022.
The formation of the tetragonal phase produces an anisotropic strain field due to the contraction and expansion of theaandcaxes against the cubic matrix.
The strain field makes {102)D022and {100)D022with the invariant lines become habit, and also drives the selective nucleation and growth of minor variants to minimize the elastic strain energy, thereby leading to the multi-variant structure.

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