Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)

2D-like indentations are performed by molecular dynamics simulation as “nanometric indentation cutting”. A 90 degree triangle rigid bcc-Fe indenter with (001) or (110) surfaces is continuously drove into single crystalline fcc-Ni and Cu with free side surface, on three different top surfaces of (001...

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Main Authors: Kisaragi YASHIRO, Shunsuke HONDA, Ryo TERADA, Keishi NAITO
Format: Article
Language:Japanese
Published: The Japan Society of Mechanical Engineers 2020-05-01
Series:Nihon Kikai Gakkai ronbunshu
Subjects:
Online Access:https://www.jstage.jst.go.jp/article/transjsme/86/885/86_20-00061/_pdf/-char/en
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author Kisaragi YASHIRO
Shunsuke HONDA
Ryo TERADA
Keishi NAITO
author_facet Kisaragi YASHIRO
Shunsuke HONDA
Ryo TERADA
Keishi NAITO
author_sort Kisaragi YASHIRO
collection DOAJ
description 2D-like indentations are performed by molecular dynamics simulation as “nanometric indentation cutting”. A 90 degree triangle rigid bcc-Fe indenter with (001) or (110) surfaces is continuously drove into single crystalline fcc-Ni and Cu with free side surface, on three different top surfaces of (001), (110) and (111) of the work materials. Despite of large difference in the elastic constants, there is little difference in the repulsive force between Ni and Cu during cutting. This is because the plastic deformation or dislocation emission immediately occurs without large elastic deformation under the 2D-like infinite-length sharp blade, in contrast to spherical indenter in 3D indentation. Ni(001) work material shows drastic change in the cutting morphology by the tool surface; cleavage cracking occurs from a line defect ahead of the (001) tool while smooth cut at the tool end is observed on the (110) tool. The key of this difference is the atomic roughness of the tool surface; the rough (001) tool leads drag and rotation of the work surface, nucleating complicated small grains around the tool. The smooth (110) tool shows growth of single grain, in which the (111) plane is parallel to the cutting direction, at the front of the contact surface. Ni work also shows various deformation mode compared to Cu work, e.g. deformation by large grain growth normal to tool surface in the (110) work and kink formation by dislocation array in the (111) work, due to the high stacking fault energy.
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spelling doaj.art-d045aa02496145a1a7e764abef44d4cd2022-12-22T03:41:37ZjpnThe Japan Society of Mechanical EngineersNihon Kikai Gakkai ronbunshu2187-97612020-05-018688520-0006120-0006110.1299/transjsme.20-00061transjsmeMolecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)Kisaragi YASHIRO0Shunsuke HONDA1Ryo TERADA2Keishi NAITO3Faculty of Engineering, Gifu UniversityNabtesco Corporation, JA Kyosai Bldg.Nabeya Bi-tech KaishaFaculty of Engineering, Gifu University2D-like indentations are performed by molecular dynamics simulation as “nanometric indentation cutting”. A 90 degree triangle rigid bcc-Fe indenter with (001) or (110) surfaces is continuously drove into single crystalline fcc-Ni and Cu with free side surface, on three different top surfaces of (001), (110) and (111) of the work materials. Despite of large difference in the elastic constants, there is little difference in the repulsive force between Ni and Cu during cutting. This is because the plastic deformation or dislocation emission immediately occurs without large elastic deformation under the 2D-like infinite-length sharp blade, in contrast to spherical indenter in 3D indentation. Ni(001) work material shows drastic change in the cutting morphology by the tool surface; cleavage cracking occurs from a line defect ahead of the (001) tool while smooth cut at the tool end is observed on the (110) tool. The key of this difference is the atomic roughness of the tool surface; the rough (001) tool leads drag and rotation of the work surface, nucleating complicated small grains around the tool. The smooth (110) tool shows growth of single grain, in which the (111) plane is parallel to the cutting direction, at the front of the contact surface. Ni work also shows various deformation mode compared to Cu work, e.g. deformation by large grain growth normal to tool surface in the (110) work and kink formation by dislocation array in the (111) work, due to the high stacking fault energy.https://www.jstage.jst.go.jp/article/transjsme/86/885/86_20-00061/_pdf/-char/enindentationcuttingtool surfacedislocationkink
spellingShingle Kisaragi YASHIRO
Shunsuke HONDA
Ryo TERADA
Keishi NAITO
Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
Nihon Kikai Gakkai ronbunshu
indentation
cutting
tool surface
dislocation
kink
title Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
title_full Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
title_fullStr Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
title_full_unstemmed Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
title_short Molecular dynamics simulation of indentation-cutting on Ni and Cu by rigid Fe tool (Focus on combination of surface structure of tool and work)
title_sort molecular dynamics simulation of indentation cutting on ni and cu by rigid fe tool focus on combination of surface structure of tool and work
topic indentation
cutting
tool surface
dislocation
kink
url https://www.jstage.jst.go.jp/article/transjsme/86/885/86_20-00061/_pdf/-char/en
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AT ryoterada moleculardynamicssimulationofindentationcuttingonniandcubyrigidfetoolfocusoncombinationofsurfacestructureoftoolandwork
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