4. B modeling#
4.1. Characteristics of modeling#
In this modeling, the simplex method is tested for crack propagation.
Level-sets are determined by solving the updating equations.
4.2. Characteristics of the mesh#
Here we use the same mesh as in modeling \(A\).
4.3. Tested sizes and results#
For each propagation step, we test the value of the stress intensity factors \({K}_{I}\) and \({K}_{\mathrm{II}}\) given by CALC_G.
4.3.1. Results on KI:#
A relative non-regression test is carried out on \({K}_{I}\) compared to \({K}_{I\mathrm{maillage}}\) with an accuracy of \(\text{5\%}\).
Identification |
Code_Aster |
Reference |
Difference ( \(\text{\%}\) ) |
|
CALC_G |
||||
KI_1 |
2.43961 10-1 |
2.43961 10-1 |
2.43961 10-1 |
2.03 10-4% |
KI_2 |
0.29056 |
2.90147 10-1 |
|
|
KI_3 |
0.3308 |
3.30840 10-1 |
3.910-4% |
|
KI_4 |
0.3759 |
3.75984 10-1 |
|
|
KI_5 |
0.43355 |
4.33606 10-1 |
7.9 10-4% |
|
KI_6 |
0.497 |
4,96975 10-1 |
|
|
KI_7 |
0.573 |
5,73785 10-1 |
|
|
KI_8 |
0.6705 |
6,70222 10-1 |
|
|
KI_9 |
0.7899 |
7,89716 10-1 |
|
|
KI_10 |
0.93757 |
9.39463 10-1 |
|
|
KI_11 |
1.1508 |
1.15201 |
1.15201 |
|
KI_12 |
1.4472 |
1.45163 |
|
|
KI_13 |
1.8923 |
1.91885 |
|
4.3.2. Results on \({K}_{\mathrm{II}}\):#
For this test, we want \({K}_{\mathrm{II}}\) to be as \({K}_{\mathrm{II}}={K}_{\mathrm{IIref}}\pm {5.10}^{-2}\). (absolute test)
Identification |
Code_Aster |
Reference |
Difference |
|
CALC_G |
||||
KII_1 |
0.04277 |
4.27722 10-2 |
3.92 10-8 |
|
KII_2 |
-0.00019 |
1.21013 10-4 |
3.1 10-4 |
3.1 10-4 |
KII_3 |
0.00864 |
7,10255 10-3 |
1,54 10-3 |
1,54 10-3 |
KII_4 |
0.00068 |
1.94683 10-3 |
0.0013 |
|
KII_5 |
0.001988 |
1.20266 10-3 |
7.85 10-4 |
|
KII_6 |
-0.0003965 |
8.82542 10-4 |
1.27 10-3 |
8.82542 10-3 |
KII_7 |
-0.001049 |
-1.23199 10-3 |
1.82 10-4 |
-1.82 10-4 |
KII_8 |
-0.01141 |
-3,54655 10-3 |
7,86 10-3 |
7,86 10-3 |
KII_9 |
0.006572 |
-4.54122 10-3 |
0.0111 |
|
KII_10 |
0.001981 |
-8,18030 10-3 |
0.01 |
|
KII_11 |
-0.038036 |
-1.55772 10-2 |
0.0224 |
|
KII_12 |
-0.012783 |
-2,31849 10-2 |
0.0104 |
|
KII_13 |
-0.02314 |
-3,52229 10-2 |
0.012 |