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A Numerical Study of Mixedmode Crack Propagation in ZnO2NiCr Functionally Graded Materials by A Hybrid PhaseField Method

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A numerical investigation of mixedmode crack propagation in functionally graded ZnO2NiCr (FG) beams using a regularized variational formulation is presented. The simulation results were compared with mixedmode three points bending experimented by Jin. et al. (Eng. Frac. Mech. 76 (2009) 1800 1810). Our numerical investigation shows that the numerical scheme based on hybrid phase field model captures well the crack propagation behavior including initial kinking angle, crack path and loaddisplacement relationship. The effect of elastic and fracture toughness mismatch on crack path behavior is also analyzed.

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A Numerical Study of Mixed-mode Crack Propagation in ZnO2/NiCr Functionally Graded Materials by A Hybrid Phase-Field Method

Phuc Minh Phama , Duc Hong Doanb, Tinh Quoc Buic, Nguyen Xuan Nguyend,

Nguyen Minh Dunge, Nguyen Binh Khieme, Nguyen Dinh Ducb,e

a

Faculty of Basic Sciences, University of Transport and Communications, Hanoi, Vietnam

b

Advanced Materials and Structures Lab, University of Engineering and Technology, VNU - Hanoi

c

Department of Civil and Environmental Engineering, Tokyo Institute of Technology, Japan

d Department of Mathematics, Mechanics and Informations - Hanoi University of Science,

VNU -Hanoi

e

Department of Mechano-Informatics, Graduate school of Information Science and Technology -

The University of Tokyo

d

Infrastructure Engineering Program, Vietnam-Japan University (VJU), VNU-Hanoi, Vietnam

Abstract

A numerical investigation of mixed-mode crack propagation in functionally graded ZnO2/NiCr (FG) beams using a regularized variational formulation is presented The simulation results were compared with mixed-mode three points bending experimented by Jin et al (Eng Frac Mech 76 (2009) 1800 1810) Our numerical investigation shows that the numerical scheme based on hybrid phase field model captures well the crack propagation behavior including initial kinking angle, crack path and load-displacement relationship The effect of elastic and fracture toughness mismatch on crack path behavior is also analyzed

Key Words: Functionally graded materials; ZnO 2 /NiCr; hybrid phase field model

1 Instructions

Functionally graded ZnO2/NiCr was fabricated

with structure of laminated ZnO2/NiCr with

different composite percentage of NiCr from 0%

to 50% (Jin, 2009) Therefore, the behaviors of

crack at interface of laminated ZnO2/NiCr are

dominated fracture mode This study aims at to

investigate the behaviors and mechanisms of a

crack propagation at interface laminated

ZnO2/NiCr by a hybrid phase field model The

effects of elastic and fracture toughness

mismatch on crack path behavior is also analyzed

2 Governing equations

In terms of phase field fracture modeling, the cracks, which can be regarded as internal discontinuities with respect to the macroscopic field, are essentially represented by a phase field

variable s bounded between 0 and 1 The phase field variable s varies continuously from 1 for undamaged materials to 0 for completely

damaged materials The hybrid (isotropic-anisotropic) phase field model for brittle fracture

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Phuc Minh Pham et al

384

is finally formulated as follows (Doan, 2016 and

Ambati, 2015):

(1) (2)

(3)

where , are the stress and strain tensors,

respectively; is the displacement field, div is

the divergence operator, and the superposed dot

represents the partial differentiation with respect

to time In Eq (2), l stands for the length scale

parameter introduced to account for the width of

the crack Gc denotes the material fracture

toughness independent of the crack speed, sis

the Laplacian of the phase field parameter, while

H introduces a strain history field of maximum

positive reference energy, 0 , obtaining in

a loading process, in order to handle the

irreversibility of the crack phase field evolution

[25]

0t 0

H ( , ) : maxxt [ , ] ( ( , ))x (4)

By only applying the phase field parameter to

the tensile part of the elastic energy density

function, 0 , we thus prohibit crack

propagation under compression, yielding:

0

1

with the elastic constant 0 ,

1

2

tr tr tr , and is the viscosity

parameter

3 Results and discussion

3.1 Crack path compared with experimental

result

We start by considering a mixed-mode experimental test of beam conducted by Jin (2009) as shown in Fig 1(a) The beam is made

of ZnO2/NiCr with the material composite of 50%ZnO2/50%NiCr The crack path and deformation are shown in Fig 1(b) Our numerical result shows that the numerical scheme based on hybrid phase field model captures well the crack propagation behavior as initial kinking angle of 10

(a) Schematic of beam and geometry parameter

(b) Deformation of beam with crack path Fig 1 Schematic of mixed-mode experimental set up and calculation crack path

3.2 Crack step-over mechanism at Compliant-to-Stiffer Interface

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Crack Propagation in ZnO 2 /NiCr Functionally Graded Materials 385

Fig 2 Schematic of three points bending

experimental set up with pre-crack located on

compliant side

(a) Loading displacement: u=0.14 mm

(b) Loading displacement: u=0.15 mm

Fig 3 Crack step-over at compliant-to-stiffer

interface

Figure 2 shows a schematic of three points

bending experimental set up with pre-crack with

length of 2.2 mm located on compliant side

Compiant and stiffer side are made of

ZnO2/NiCr with the material composite of

50%ZnO2/50%NiCr and ZnO2, respectively

Interestingly, the crack is generated firstly at

stiffer side than propagates to compliant side as

shown in Fig 3 This mechanism is called crack

step-over, which occurs when a crack propagates from compliant-to-stiffer interface It

is worth noting that, although crack step-over has been predicted in Leguillon (2013), it is first time visualized by numerical simulation in this work

3.3 Crack branching at Stiffer-to-Compliant Interface

Next, we consider a case when pre-crack located

at stiffer side A calculation set up is same as in Fig 2 with only a change of location of stiffer side and compliant side Calculation results are shown in Fig 4 As crack propagates to stiffer-to-compliant interface, crack is arrested and branching at the interface

(a) Loading displacement: u=0.26 mm

(b) Loading displacement: u=0.28 mm

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Phuc Minh Pham et al

386

(c) Loading displacement: u=0.6 mm

Fig 4 Crack branching at stiffer-to-compliant

interface

4 Conclusions

In this study, investigate the behavior and

mechanism of a crack propagation at interface

laminated ZnO2/NiCr by a hybrid phase field

model Simulation results demonstrates the

crack step-over mechanism at interface of

compliant-to-stiffer At interface of

stiffer-to-compliant interface, crack is arrested and

branching

Acknowledgement: This research is funded by

Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number 107.02-2015.03 and ISPS-Japan The authors are grateful for this support

References

Ambati, M et al (2015) , A phase-field model for ductile fracture at finite strains and its experimental verification, Comput Mech 57 pp 149-267

Doan, HD et al (2016), Hybrid Phase Field Simulation of Dynamic Crack Propagation in

Functionally Graded Glass-Filled Epoxy, Composites Part B 99 pp 266-276

Leguillon, D et al (2013), The strengthening effect caused by an elastic contrast part I: the bimaterial

case Int J Fract 179 pp 157 167

Jin, X et al (2009), Experimental investigation of the mixed-mode crack propagation in ZrO2/NiCr

functionally graded materials, Engineering Fracture Mechanics 76 pp 1800 1810

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437

Tinh Quoc Bui 253, 259, 265, 383

Duc Hong Doan 253, 259, 265, 383

Van Manh Hoang 84, 138, 154, 161

Nguyen Dinh Duc 253, 259, 265, 292, 302,

310, 383

Nguyen Quang Hoang 107, 114, 207 Nguyen Quang Huan 334, 393

Nguyen Van Khang 124, 167, 207

Khoa Viet Nguyen 217, 225, 233, 387 Nguyen Dinh Kien 269, 326, 334, 393, 422

Ngoc Linh Nguyen 132, 154

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438 Authors Index

Nguyen Van Long (UCE) 409

Van Long Nguyen (UET) 132

Nguyen Xuan Nguyen 265, 383

Nguyen Thi Phuong 342, 355, 429

Quang Van Nguyen 225, 233

Minh Triet Nguyen 132, 138

Ngoc Viet Nguyen 84, 132, 138, 154

Manh Thang Pham 84, 132, 138 154, 161

Vu Hoai Nam 342, 355, 429

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Steering Committee

Nguyen Huu Duc, Nguyen Viet Ha, Duong Ngoc Hai, Nguyen Hoa Thinh

Program Committee

Chairman: Nguyen Dong Anh

Vice Chairman: Nguyen Dinh Duc, Dinh Van Manh

Dao Huy Bich, Le Van Canh, Truong Huu Chi, Doan Minh Chung, Dao Van Dung, Duc Pham (UK), Nguyen Van Diep, Dimitri V Georgievskii (Russia), Duong Ngoc Hai, Nguyen Xuan Hung, Cao The Huynh, Le Xuan Huynh, Seung Chul Jung (Korea), Kazuyoshi Fushinobu (Japan), Nguyen Van Khang, Nguyen Tien Khiem, Kim Chun-Gon (Korea), Nguyen Thi Viet Lien, Nguyen Cao Menh, Nguyen Van Pho, No-Cheol Park (Korea), Dinh Van Phong, Pham Hong Phuc, Do Sanh, Suong H Van (Canada), Pham Manh Thang, Truong Tich Thien, Tran Ich Thinh, Bui Dinh Tri, Nguyen Thoi Trung, Pham Anh Tuan, Tuan D Ngo (Australia), Pham Chi Vinh, Hui-Shen Shen (China)

Organising Committee

Chairman: Nguyen Dinh Duc

Vice Chairman: Nguyen Viet Khoa, Pham Manh Thang

Dang The Ba, Tran Mau Danh, Tran Thi Thu Ha, Pham Duy Hung, Seung Chul Jung (Korea), Nguyen Ha Nam, Bui Trung Ninh, Nguyen Hoang Quan, Nguyen Phuong Thai, Pham Minh Trien

Secretariat

Chairman: Dao Nhu Mai

Vu Thi Thuy Anh, Nguyen Ngoc Linh, Phan Thi Cam Ly, Hoang Van Manh, Tran Quoc Quan, Nguyen Cao Son, Nguyen Ngoc Viet, Tran Hai Yen

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