Title: Crack growth problem
1Crack growth problem in a riveted lap-joint panel
Paulo F P de Matos, Pedro M G P Moreira, Paulo M
S T de Castro IDMEC, University of Porto,
Portugal
2Objectives
- Crack growth prediction in complex structures
- 2) Compare numerical/analytical results with the
- experimental measurements.
3 Specimen geometry
Rivet type MS20426D5-6 in Al
2017-T31
Specimen BJ3, UPisa
Load conditions
Al 2024-T351
smax110 MPa R0.1
4Lap-joint mesh
Lap-joint mesh / layer1 and layer 2
Riveted lap joint mesh, where triangles represent
rivets
5Lap-joint panel stress analysis
- Boundary conditions
- - Top edged of layer 1 fixed along
- X and Y directions.
- The bottom edge of layer 2 was
- fixed along X and a constant
- tensile stress of 110 MPa was
- applied.
y
x
6Crack tips location and crack shape
Inspected sites for crack initiation
Crack shape
7Crack scenario at 137950 cycles
Stress sy at 137950 cycles near crack tips 1 to 4
Crack scenario at 137950 cycles
8Algorithm for crack propagation
C7.46E-8 m3.333
9Comparison of results
Continuous lines represent the FRANC2D/L
results Bullets concern to experimental results
10Comparison of results
Continuous lines represent the FRANC2D/L
results Bullets concern to experimental results
11Comparison of results
Continuous lines represent the FRANC2D/L
results Bullets concern to experimental results
12Final remarks
- The main conclusions of the present work are
- 1) Crack growth modeling was done in a lap-joint
panel from 132150 to 138450 cycles - 2) A good agreement was found between the
experimentation and the prediction of FRANC2D/L
based on the Paris Law. - Although the good results obtained there are
important - limitations that must be mentioned
- 1) As previously mentioned cracks grow with an
elliptical shape and not as through cracks
13Final remarks
2) The rivets are treated as spring elements. It
is only a simplification that has some
limitations. The typical stress distribution
of a hole is not considered 3) FRANC2D/L
allows only a 2D model of a joint, so the
secondary bending expected in a typical lap joint
cannot be modelled.