PSI - Issue 13

Katharina Dibblee et al. / Procedia Structural Integrity 13 (2018) 322–327 Katharina Dibblee et al./ Structural Integrity Procedia 00 (2018) 000 – 000

324

3

Fig. 2. Crack propagation in a 3-dimensional fracture mechanical graded structure: (a) application of the new 3D-criterion, (b) determination of the relevant stress function

In order to calculate the required contact of the two functions, the stress at the crack front is first converted to a cyclic stress function and afterwards compared with the local material function. For this purpose, the maximal principle stress σ 1 ' is converted into a cyclic stress function

  

2 1

2 3

  

  

  

   

  

Δ

cos Δ K

sin Δ K

' 1

2

σ

  r

2

cos

I

II

2

2

   

2

  

   

2 3

  

   

(1).

  

cos Δ K

sin Δ K

Δ 4

2

2 III

K

I

II

2

The relevant stress function which shows the first contact with the material function results from the consideration of the two stress functions f 1 (  K I th,3D ) and f 2 (  K I th,3D ) from Fig. 2 (b). These two functions are determined as a function of the local threshold  K I,th for the material ranges M1 and M2 as well as the kinking angle φ 0 and the grading angle φ M .

  

  

B A A B A B

0 

2 1

   2 1 3

  

  

  

   

  

  0 

  

  0 

Δ

Δ

th,3D I

2 0

K

K

cos

cos

sin

I,th 0

2

2

 

1

       

2

2

  

   

B A A

2 1 3   

  

   

  

  

  

(2)

  0 

2 0

cos

sin

4

2

1

 

 

  

B A A

  

2 1

   2 1 3

     

  

  

   

  

  M 

  

  M 

Δ

Δ

th,3D I

2 M

K

K

cos

cos

sin

M

I,th M

2

2

 

1

       

2

2

B A A

B A B

  

   

2 1 3

  

   

  

  

  

  M 

(3)

2 M

cos

sin

4

 

 

2

1

A and B represent the mixed-mode ratios:

II Δ Δ Δ Δ  

III Δ Δ Δ Δ  

K K K K

K K K K

A

B

and

(4).

I

II

III

I

II

III

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