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Molecular Dynamics Study on Drawing Process of Metallic Wire: Effect of Nano-sized Texture on Friction and Plasticity Sustainable Triborogy Conference 2017 Amami (STCA2017), Oct 13- 16, 2017, Amami-Oshima, Kagoshima, Japan Summary: In this study, possibility of nano-sized wiredrawing was studied by using molecular dynamics (MD) simulations. In particular, effect of nano-sized texturing (Ntxt: here, single type of periodic grooves perpendicular to sliding direction) on die surface was investigated. Friction behavior is continuous stick-and-slip. Larger-sized Ntxt results in smaller shear stress on the materials, and accordingly smaller coefficient of friction in sliding. However it seems it largely depends on stability of Ntxt structure. In designing, the structure of Ntxt should be optimized as for size, shape as well as arrangement. 2017/10/14 K.Saitoh (C) <Last modified 2017/10/13> Background (open questions) Can wiredrawing process (plastic working) perform in nano-sized scale? (Possible) Will nano-sized texturing (new idea) reduce friction between die and wire? How microscopic plasticity (i.e. dislocation) in drawing is affected by nano-sized texturing? (in particular, from atomistic point of view) Molecular dynamics model for Nano-sized wiredrawing Materials: iron and steel FS potential (many-body type) Velocities of entrance and exit are determined by conservation of volume law. Interaction between die and wire is weakened by ω<1 (artificial lubrication model). Nano-sized texturing (Ntxt) set-up for MD analysis = + Pitch ratio (non-dimensional factor) DXA (Dislocation Extraction Algorithm) Wiredrawing process (conventional) die wire/ bar/pipe Key factors : reduction of area, wire velocity, lubrication, material dislocation line Fig. Example view obtained in dislocation analysis of nano-sized wiredrawing by using DXA method (drawing direction <110>,Die semi-angle α=5 deg, Velocity V out =10 m/s, No texturing) Detecting lattice defects by CNA Determining and indicating dislocation line Identifying Burger’s circuit Stukowski, A., et al., Model.Simul.Mater.Sci. Eng.,18, 025016 (2010). Patching surface around dislocation Flow of DXAOvitoTable Computation condition for nano-sized wiredrawing Drawing direction <100> <110> <111> The number of atoms [-] 211757 214285 209745 Cell size in x,y,z [nm] 9.88, 9.88, 13.8 Velocity , [m/s] 21.9, 30.0 Diameter , [nm] 13.8, 12.8 Length of die 0 [nm] 4.12 Lubrication factor ω 0.01 Fig. MD models with nano-sized texture (NTxt) (a)Pattern 1 (b)Pattern 2 (c)Pattern 3 (d)Geometric parameters of NTxts Simple Flat surface contact MD model with Ntxt shear stress τ yz normal stress σ z (compressive) σ z <0 τ yz >0 τ yz >0 σ z <0 y x z stress components in sliding motion Mechanism of Ntxt break force failure case Large Ntxt stiff deformable force small Ntxt stiff deformable force Fig. Averaged stress τ yz 0 0.5 1 1.5 2 Pattern1 Pattern2 Pattern3 Shear stress[GPa] No Ntxt small Ntxt large Ntxt Fig. coefficient of friction μ = τ yz /σ z 0 0.05 0.1 0.15 0.2 Pattern1 Pattern2 Pattern3 Coefficient of friction[-] No Ntxt small Ntxt large Ntxt Fig. Distribution of radial stress (σ r ) and detected dislocation lines in α-Fe wire model, viewing from drawing direction Fig. Time transition of stresses we are trying to apply Ntxt to wiredrawing model, so... Results (examples) Results (Ntxt) Discussion (Ntxt) Ken-ichi Saitoh, Department of Mechanical Engineering, Kansai University 3-3-35 Yamate-cho, Suita, Osaka, 564-8680 Japan Tomohiro Sato, Koki Yoshida, Kazuki Yokohama, Kansai University Masanori Takuma, Yoshimasa Takahashi, Kansai University Stiffness of Ntxt depends on texture size. Large Ntxt can be deformed by smaller force. Too large Ntxt does not endure the force (plasticity, buckling). Large Ntxt is subjected to larger normal force per one. Optimized size and structure of Ntxt should be designed. Pattern 1 Pattern 2 Pattern 3 The number of atoms 13056 12672 12288 Cell size in x,y,z [nm] 13.728, 4.576, 2.288 Velocity [m/s] 100.0 Depth d [nm] - 0.143 0.286 Width w [nm] - 0.286 0.572 Pitch p [nm] - 0.572 1.144 Temperature T [K] 300.0 Table Calculation condition NTxt model by MD Dislocation analysis in MD (wiredrawing model) Total energy = + 1 2 Lubrication model for FS potentialelectron density = ω Many-body term =

Molecular Dynamics Study on Drawing Process of …...Molecular Dynamics Study on Drawing Process of Metallic Wire: Effect of Nano-sized Texture on Friction and Plasticity Sustainable

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Page 1: Molecular Dynamics Study on Drawing Process of …...Molecular Dynamics Study on Drawing Process of Metallic Wire: Effect of Nano-sized Texture on Friction and Plasticity Sustainable

Molecular Dynamics Study on Drawing Process of Metallic Wire: Effect of Nano-sized Texture on Friction and Plasticity

Sustainable Triborogy Conference 2017 Amami (STCA2017), Oct 13-16, 2017, Amami-Oshima, Kagoshima, Japan

Summary: In this study, possibility of nano-sized wiredrawing was studied by using molecular dynamics (MD) simulations. In particular, effect of nano-sized texturing (Ntxt: here, single type of periodic grooves perpendicular to sliding direction) on die surface was investigated. Friction behavior is continuous stick-and-slip. Larger-sized Ntxt results in smaller shear stress on the materials, and accordingly smaller coefficient of friction in sliding. However it seems it largely depends on stability of Ntxt structure. In designing, the structure of Ntxt should be optimized as for size, shape as well as arrangement.

2017/10/14 K.Saitoh (C) <Last modified 2017/10/13>

Background (open questions) Can wiredrawing process (plastic working) perform in nano-sized scale? (Possible)Will nano-sized texturing (new idea) reduce friction between die and wire? How microscopic plasticity (i.e. dislocation) in drawing is affected by nano-sized

texturing? (in particular, from atomistic point of view)

Molecular dynamics model for Nano-sized wiredrawing • Materials: iron and steel• FS potential (many-body type)• Velocities of entrance and exit are determined by conservation of volume law.• Interaction between die and wire is weakened by ω<1 (artificial lubrication model).

Nano-sized texturing (Ntxt) set-up for MD analysis

𝑃𝑃 =𝑤𝑤 + 𝑖𝑖𝑑𝑑

Pitch ratio (non-dimensional factor)

DXA (Dislocation Extraction Algorithm)

Wiredrawing process (conventional)

die

wire/ bar/pipe

Key factors: reduction of area, wire velocity, lubrication, material

dislocation line Fig. Example view obtained in dislocation analysis of nano-sized wiredrawing by using DXA method(drawing direction <110>,Die semi-angleα=5 deg, VelocityVout=10 m/s, No texturing)

Detecting lattice defects by CNA

Determining and indicating dislocation line

Identifying Burger’s circuit

Stukowski, A., et al., Model.Simul.Mater.Sci.Eng.,18, 025016 (2010).

Patching surface around dislocation

Flow of DXA(Ovito)

Table Computation condition for nano-sized wiredrawingDrawing direction <100> <110> <111>

The number of atoms [-] 211757 214285 209745Cell size in x,y,z [nm] 9.88, 9.88, 13.8

Velocity 𝑉𝑉𝑖𝑖𝑖𝑖,𝑉𝑉𝑜𝑜𝑜𝑜𝑜𝑜 [m/s] 21.9, 30.0Diameter 𝐷𝐷𝑖𝑖𝑖𝑖,𝐷𝐷𝑜𝑜𝑜𝑜𝑜𝑜 [nm] 13.8, 12.8

Length of die 𝐿𝐿0 [nm] 4.12Lubrication factor ω 0.01

Fig. MD models with nano-sized texture (NTxt) (a)Pattern 1 (b)Pattern 2 (c)Pattern 3 (d)Geometric parameters of NTxts

Simple Flat surface contact MD model with Ntxt

shear stress τyz

normal stress σz(compressive)

σz<0

τyz>0

τyz>0σz<0

yx

z

stress components in sliding motion

Mechanism of Ntxt

break

force

failurecase

Large Ntxt

stiff

deformableforce

small Ntxt

stiff

deformable force

Fig. Averaged stress τyz

0

0.5

1

1.5

2

Pattern1 Pattern2 Pattern3

Shea

r str

ess[

GPa]

No Ntxt small

Ntxt largeNtxt

Fig. coefficient of friction μ = τyz/σz

0

0.05

0.1

0.15

0.2

Pattern1 Pattern2 Pattern3

Coef

ficie

nt o

f fr

ictio

n[-] No

Ntxt small Ntxt

largeNtxt

Fig. Distribution of radial stress (σr) and detected dislocation lines in α-Fe wire model, viewing from drawing direction

Fig. Time transition of stresses

we are trying to apply Ntxtto wiredrawing model, so...

Results(examples)

Results (Ntxt)

Discussion (Ntxt)

Ken-ichi Saitoh, Department of Mechanical Engineering, Kansai University3-3-35 Yamate-cho, Suita, Osaka, 564-8680 JapanTomohiro Sato, Koki Yoshida, Kazuki Yokohama, Kansai UniversityMasanori Takuma, Yoshimasa Takahashi, Kansai University

Stiffness of Ntxt depends on texture size.

Large Ntxt can be deformed by smaller force.

Too large Ntxtdoes not endure the force (plasticity, buckling).

Large Ntxt is subjected to larger normal force per one.

Optimized size and structure of Ntxt should be designed.

Pattern 1 Pattern 2 Pattern 3The number of atoms 13056 12672 12288Cell size in x,y,z [nm] 13.728, 4.576, 2.288

Velocity 𝑉𝑉 [m/s] 100.0Depth d [nm] - 0.143 0.286Width w [nm] - 0.286 0.572Pitch p [nm] - 0.572 1.144

Temperature T [K] 300.0

Table Calculation condition NTxt model by MD

Dislocation analysis in MD (wiredrawing model)

Total energy

𝐸𝐸 = �𝑖𝑖

𝐹𝐹𝑖𝑖 𝜌𝜌 +12�𝑗𝑗≠𝑖𝑖

𝜙𝜙𝑖𝑖𝑗𝑗 𝑟𝑟𝑖𝑖𝑗𝑗

Lubrication model (for FS potential)

electron density

𝜌𝜌𝑖𝑖 = �𝑗𝑗≠𝑖𝑖

ω 𝜌𝜌 𝑟𝑟𝑖𝑖𝑗𝑗

Many-bodyterm 𝐹𝐹 𝜌𝜌 = 𝜌𝜌