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Global energy minimization for multiple fracture growth

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(1)

Global energy minimization for multiple fracture growth

Danas Sutula

Prof. Stephane Bordas & Dr. Pierre Kerfriden

(10/12/13)

(2)

Discretization: XFEM

Extended Finite Element Method (XFEM)

• Introduced by Ted Belytschko et al. (1999) for elastic problems

T. Belytschko, Northwestern Univeristy

Fracture process (>300 cracks)

vertical tensile loading

Fracture of “XFEM” using XFEM

pressure driven crack propagation

(3)

Discretization: XFEM

Approximation function :

singular tip enrichment discontinuous

enrichment standard part

Enriched nodes - “Heaviside”

- ”crack tip”

(4)

Crack propagation: traditional approach

Evaluation of stress intensity factors (SIF)

• The interaction integral (Yau 1980)

Crack growth criterion for mixed mode fracture

• Direction that maximises the energy release (Nuismer 1975)

Crack growth direction

• orthogonal to maximum hoop stress

 









8

4 tan 1 2 ,

2 1

II I II

II I II

I

c K

K K K sign

K K

K

2 2

2

c II

I K K

K  





d

x U q

x u x

I u

j j

i ij

i

ij 1

) 2 1 ( int 1

) 1 ( ) 2 ( 1

) 2 ( ) 1 ( )

2 1

(

(1) (2) (1) (2)

(1 2)

*

2

K K I K

E KI I II II

(1) – from current solution (2) – known auxiliary solution

(5)

Crack propagation: optimization of directions

• Energy release rate w.r.t crack increment direction:

• The rates of the energy release rate are given by:

• where, in a discrete setting, the potential energy is:

(6)

Crack propagation: optimization of directions

• The discrete potential energy:

• The discrete energy release rate:

• The rates of the energy release rate

(where: )

(where: )

(7)

Crack propagation: optimization of directions

• The discrete potential energy:

• The discrete energy release rate:

• The rates of the energy release rate

𝟎

(where: )

(where: )

(8)

Crack propagation: optimization of directions

• The discrete potential energy:

• The discrete energy release rate:

• The rates of the energy release rate

𝟎

(where: )

(where: )

(9)

Crack propagation: optimization of directions

• The discrete potential energy:

• The discrete energy release rate:

• The rates of the energy release rate

𝟎

(where: )

(where: )

expensive

remote interaction

(10)

Implementation

(11)

Implementation

(12)

• The discrete potential energy:

• The discrete energy release rate:

• The rates of the energy release rate

𝟎

(where: )

(where: )

Implementation

(13)

Updated directions:

Implementation

(14)

Square plate in pure mode-I loading with varying increment angle

Potential energy vs. crack increment angle -75o

0o

Verification: energy release rates

(15)

Square plate in pure mode-I loading with varying increment angle

mesh= 50 x 50, 𝑟𝑡𝑖𝑝 = 2.5ℎ𝑒, ∆𝑎𝑖𝑛𝑐 = 0.1

Verification: energy release rates

Energy release rate vs. crack increment angle Rate of energy release vs. increment angle

(16)

Square plate in pure mode-I loading with varying increment angle

mesh= 100 x 100, 𝑟𝑡𝑖𝑝 = 5.0ℎ𝑒, ∆𝑎𝑖𝑛𝑐 = 0.1

Verification: energy release rates

Energy release rate vs. crack increment angle Rate of energy release vs. increment angle

(17)

Square plate in pure mode-I loading with varying increment angle

mesh= 200 x 200, 𝑟𝑡𝑖𝑝 = 10.0ℎ𝑒, ∆𝑎𝑖𝑛𝑐 = 0.1

Verification: energy release rates

Energy release rate vs. crack increment angle Rate of energy release vs. increment angle

(18)

• Geometrical tip enrichment ( )

• Topological enrichment ( )

mesh = 200 x 200, 𝑟𝑡𝑖𝑝 = 10.0ℎ𝑒 mesh = 100 x 100, 𝑟𝑡𝑖𝑝 = 5.0ℎ𝑒

mesh = 50 x 50, 𝑟𝑡𝑖𝑝 = 2.5ℎ𝑒 𝑟𝑒𝐻𝑠 𝐿2 = 0.130

𝑟𝑒𝐻𝑠 𝐿2 = 0.076 𝑟𝑒𝐻𝑠 𝐿2 = 0.044

Verification: energy release rates

(19)

• Geometrical tip enrichment ( )

• Topological enrichment ( )

mesh = 200 x 200, 𝑟𝑡𝑖𝑝 = 10.0ℎ𝑒 mesh = 100 x 100, 𝑟𝑡𝑖𝑝 = 5.0ℎ𝑒

mesh = 50 x 50, 𝑟𝑡𝑖𝑝 = 2.5ℎ𝑒 𝑟𝑒𝐻𝑠 𝐿2 = 0.130

𝑟𝑒𝐻𝑠 𝐿2 = 0.076 𝑟𝑒𝐻𝑠 𝐿2 = 0.044

mesh = 100 x 100, ∆𝑎𝑖𝑛𝑐 = 0.050

mesh = 50 x 50, ∆𝑎𝑖𝑛𝑐 = 0.100 𝑟𝑒𝐻𝑠 𝐿2 = 0.130 𝑟𝑒𝐻𝑠 𝐿2 = 0.134 𝑟𝑒𝐻𝑠 𝐿2 = 0.139 mesh = 200 x 200, ∆𝑎𝑖𝑛𝑐 = 0.025

Verification: energy release rates

(20)

Results: Double cantilever problem

(21)

Results: Double cantilever problem

F

F

(22)

Results: Double cantilever problem

F

F

(23)

Results: Double cantilever problem

(24)

Results: Double cantilever problem

(25)

Results: Double cantilever problem

(26)

Results: Two Edge Cracks

(27)

Results: Two Edge Cracks

(28)

Results: Two Edge Cracks

(29)

Results: Two cracks protruding from holes

(30)

Results: Two cracks protruding from holes

(31)

Results: Two cracks protruding from holes

(32)

Results: 5 randomly distributed cracks

(33)

Results: 5 randomly distributed cracks

(34)

Results: 5 randomly distributed cracks

(35)

Results: 5 randomly distributed cracks

(36)

What’s next

• Energy release rates w.r.t crack increment length:

,

 Robust crack growth criterion for multiple fractures

 Global energy minimization w.r.t. both ,

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