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Atomistic simulation of an f.c.c./b.c.c. interface in NiCr alloys

The embedded atom method is applied to study the atomic structure and energy of an f.c.c./b.c.c. interface in NiCr. The two phases are oriented in a Kurdjumov-Sachs orientation relationship, and the interface considered is the (1 2̄ 1) f habit plane adopted by precipitate laths of the b.c.c. phase....

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Published in:Acta materialia 1997-11, Vol.45 (11), p.4415-4421
Main Authors: Chen, J.K., Farkas, D., Reynolds, W.T.
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Language:English
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cited_by cdi_FETCH-LOGICAL-c459t-253a5673053eb2f4a43bd910009c10252a06d45d844f35884737d833d15eadde3
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description The embedded atom method is applied to study the atomic structure and energy of an f.c.c./b.c.c. interface in NiCr. The two phases are oriented in a Kurdjumov-Sachs orientation relationship, and the interface considered is the (1 2̄ 1) f habit plane adopted by precipitate laths of the b.c.c. phase. The interfacial energy and coherent strain energy at 0 K are calculated for boundaries between an f.c.c. NiCr solid solution and b.c.c. Cr. The calculated interfacial energy varies from 216 mJ/m 2 when the f.c.c. phase is pure Ni to 200 mJ/m 2 when the f.c.c. phase is Ni50 at. % Cr. Atomic relaxations appear limited to atoms in contact with the interphase boundary. Most of the interfacial energy is attributed to the structural difference across the f.c.c./b.c.c. boundary, and the chemical contribution to the energy is estimated to be less than 20% of the total energy. The value of the calculated energies and the widespread occurrence of the (1 2̄ 1) f habit plane in a variety of alloy systems indicate this boundary orientation has a relatively low interfacial energy.
doi_str_mv 10.1016/S1359-6454(97)00159-6
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The two phases are oriented in a Kurdjumov-Sachs orientation relationship, and the interface considered is the (1 2̄ 1) f habit plane adopted by precipitate laths of the b.c.c. phase. The interfacial energy and coherent strain energy at 0 K are calculated for boundaries between an f.c.c. NiCr solid solution and b.c.c. Cr. The calculated interfacial energy varies from 216 mJ/m 2 when the f.c.c. phase is pure Ni to 200 mJ/m 2 when the f.c.c. phase is Ni50 at. % Cr. Atomic relaxations appear limited to atoms in contact with the interphase boundary. Most of the interfacial energy is attributed to the structural difference across the f.c.c./b.c.c. boundary, and the chemical contribution to the energy is estimated to be less than 20% of the total energy. 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The value of the calculated energies and the widespread occurrence of the (1 2̄ 1) f habit plane in a variety of alloy systems indicate this boundary orientation has a relatively low interfacial energy.</description><subject>Applied sciences</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Exact sciences and technology</subject><subject>Martensitic transformations</subject><subject>Materials science</subject><subject>Metals. 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The two phases are oriented in a Kurdjumov-Sachs orientation relationship, and the interface considered is the (1 2̄ 1) f habit plane adopted by precipitate laths of the b.c.c. phase. The interfacial energy and coherent strain energy at 0 K are calculated for boundaries between an f.c.c. NiCr solid solution and b.c.c. Cr. The calculated interfacial energy varies from 216 mJ/m 2 when the f.c.c. phase is pure Ni to 200 mJ/m 2 when the f.c.c. phase is Ni50 at. % Cr. Atomic relaxations appear limited to atoms in contact with the interphase boundary. Most of the interfacial energy is attributed to the structural difference across the f.c.c./b.c.c. boundary, and the chemical contribution to the energy is estimated to be less than 20% of the total energy. 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subjects Applied sciences
Cross-disciplinary physics: materials science
rheology
Exact sciences and technology
Martensitic transformations
Materials science
Metals. Metallurgy
Phase diagrams and microstructures developed by solidification and solid-solid phase transformations
Physics
title Atomistic simulation of an f.c.c./b.c.c. interface in NiCr alloys
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