The substructure of Ni3Mo due to ordering

E. Ruedl; S. Amelinckx

doi:10.1016/0025-5408(69)90092-0

The substructure of Ni₃Mo due to ordering

E. Ruedl, S. Amelinckx

Research output › peer-review

Abstract

The substructure of Ni₃Mo resulting from ordering consists of anti-phase boundaries and twins. The quenched-in FCC phase exhibits short range order of the same type as in Ni₄Mo. The short range order can be destroyed by irradiation. The transition from the FCC stacking to the ordered pseudo-hexagonal stacking (orthorhombic) is presumably a shear transformation as can be deduced from the orientation relationship. The stacking fault energy is small in the FCC + NiMo phase, as can be concluded from the presence of large extended nodes.

Original language	English
Pages (from-to)	361-368
Number of pages	8
Journal	Materials Research Bulletin
Volume	4
Issue number	6
DOIs	https://doi.org/10.1016/0025-5408(69)90092-0
State	Published - Jun 1969

ASJC Scopus subject areas

General Materials Science
Condensed Matter Physics
Mechanics of Materials
Mechanical Engineering

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10.1016/0025-5408(69)90092-0

Cite this

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title = "The substructure of Ni3Mo due to ordering",

abstract = "The substructure of Ni3Mo resulting from ordering consists of anti-phase boundaries and twins. The quenched-in FCC phase exhibits short range order of the same type as in Ni4Mo. The short range order can be destroyed by irradiation. The transition from the FCC stacking to the ordered pseudo-hexagonal stacking (orthorhombic) is presumably a shear transformation as can be deduced from the orientation relationship. The stacking fault energy is small in the FCC + NiMo phase, as can be concluded from the presence of large extended nodes.",

author = "E. Ruedl and S. Amelinckx",

year = "1969",

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AB - The substructure of Ni3Mo resulting from ordering consists of anti-phase boundaries and twins. The quenched-in FCC phase exhibits short range order of the same type as in Ni4Mo. The short range order can be destroyed by irradiation. The transition from the FCC stacking to the ordered pseudo-hexagonal stacking (orthorhombic) is presumably a shear transformation as can be deduced from the orientation relationship. The stacking fault energy is small in the FCC + NiMo phase, as can be concluded from the presence of large extended nodes.

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