Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Residual Strength and Fatigue Lifetime of ... - Solid Mechanics Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
3.6 Conclusion In this chapter the compressive failure of foam cored sandwich panels containing a face/core circular debond was experimentally and numerically investigated. Sandwich panels with glass/polyester face sheets and H130, H250 and PMI foam cores were tested in a specially designed test rig. All debonded panels failed by the propagation of the debond to the edges of the panels. All intact panels with H130 and H250 cores failed by the compressive failure of a face sheet very close to the wooden inserts, which can be attributed to additional peeling stresses arising due to the junction between the insert and the core and to a slight unintentional mismatch between the core and insert thicknesses. Intact panels with PMI core failed by a combination of shear crimping and global buckling. MMB characterisation tests were conducted to measure the fracture toughness of the face/core interface for a span of mode-mixity phase angles. Results showed increasing fracture toughness for increasing magnitude of the phase angle. A large scatter was observed in the fracture toughness results due to brittleness of the core material, different manufacturing defects and dissimilarity in crack propagation paths at the face/core interface. Instability and crack propagation loads of the panels were estimated based on geometrically nonlinear finite element analysis and linear elastic fracture mechanics. A numerical scheme similar to the one developed in Chapter 2, based on submodelling was used for the simulations. In some of the panels the FEA predictions are up to 46% higher than the experimental ones, which can be attributed to the large scatter in the measured fracture toughness using MMB fracture toughness results and differing crack tip details between the panels and the MMB specimens due to mechanical releasing of the debonded area. However, in most of the panels better agreement, up to 20% deviation, is observed between numerical and experimental results. To investigate the debond propagation path in the tested panels, some of the panels were cut and it was observed that the debond propagation path is similar between the panels and the MMB specimens. It was observed that in the panels and the MMB specimens with PMI core and panels with H130 core, the debond kinks into the core and propagates beneath the face/core interface. However, in the MMB specimens with H130 core two different crack growth paths were observed. In the H130 MMB specimens with the mode-mixity phase angle of 0° >> -20° (similar to the panels), the crack path was located below the face/core interface. However, when the magnitude of the mode-mixity phase angle was increased to -25° >> -65°, the crack path was directly in the face/core interface. In the panels and the MMB specimens with H250 core the debond propagates directly in the interface. This may be explained by the higher fracture toughness of the H250 core compared to H130 and PMI cores. Fibre bridging was observed after more than 4- 5 mm crack growth in the MMB specimens and panels with H250 core. The similarity between the debond propagation paths in the MMB specimens and the panels refutes the role of the different propagation paths in the inaccuracy of the determined debond propagation loads. 60
To examine the effect of initial imperfection magnitude on the behaviour of the panels, panels with different initial imperfection magnitudes were analysed. It was shown that the initial imperfection magnitude has no significant effect on the energy release rate. Regarding the modemixity the effect becomes less important at higher loads. Finally, based on experimental and numerical results, the strength reduction factor Rl was plotted against debond diameter. The plot is tentative due to the uncertainties regarding the intact strengths as well as the differences between test and analysis results. 61
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3.6 Conclusion<br />
In this chapter the compressive failure <strong>of</strong> foam cored s<strong>and</strong>wich panels containing a face/core<br />
circular debond was experimentally <strong>and</strong> numerically investigated. S<strong>and</strong>wich panels with<br />
glass/polyester face sheets <strong>and</strong> H130, H250 <strong>and</strong> PMI foam cores were tested in a specially<br />
designed test rig. All debonded panels failed by the propagation <strong>of</strong> the debond to the edges <strong>of</strong> the<br />
panels. All intact panels with H130 <strong>and</strong> H250 cores failed by the compressive failure <strong>of</strong> a face<br />
sheet very close to the wooden inserts, which can be attributed to additional peeling stresses<br />
arising due to the junction between the insert <strong>and</strong> the core <strong>and</strong> to a slight unintentional mismatch<br />
between the core <strong>and</strong> insert thicknesses. Intact panels with PMI core failed by a combination <strong>of</strong><br />
shear crimping <strong>and</strong> global buckling. MMB characterisation tests were conducted to measure the<br />
fracture toughness <strong>of</strong> the face/core interface for a span <strong>of</strong> mode-mixity phase angles. Results<br />
showed increasing fracture toughness for increasing magnitude <strong>of</strong> the phase angle. A large<br />
scatter was observed in the fracture toughness results due to brittleness <strong>of</strong> the core material,<br />
different manufacturing defects <strong>and</strong> dissimilarity in crack propagation paths at the face/core<br />
interface.<br />
Instability <strong>and</strong> crack propagation loads <strong>of</strong> the panels were estimated based on geometrically nonlinear<br />
finite element analysis <strong>and</strong> linear elastic fracture mechanics. A numerical scheme similar<br />
to the one developed in Chapter 2, based on submodelling was used for the simulations. In some<br />
<strong>of</strong> the panels the FEA predictions are up to 46% higher than the experimental ones, which can be<br />
attributed to the large scatter in the measured fracture toughness using MMB fracture toughness<br />
results <strong>and</strong> differing crack tip details between the panels <strong>and</strong> the MMB specimens due to<br />
mechanical releasing <strong>of</strong> the debonded area. However, in most <strong>of</strong> the panels better agreement, up<br />
to 20% deviation, is observed between numerical <strong>and</strong> experimental results. To investigate the<br />
debond propagation path in the tested panels, some <strong>of</strong> the panels were cut <strong>and</strong> it was observed<br />
that the debond propagation path is similar between the panels <strong>and</strong> the MMB specimens. It was<br />
observed that in the panels <strong>and</strong> the MMB specimens with PMI core <strong>and</strong> panels with H130 core,<br />
the debond kinks into the core <strong>and</strong> propagates beneath the face/core interface. However, in the<br />
MMB specimens with H130 core two different crack growth paths were observed. In the H130<br />
MMB specimens with the mode-mixity phase angle <strong>of</strong> 0° >> -20° (similar to the panels), the<br />
crack path was located below the face/core interface. However, when the magnitude <strong>of</strong> the<br />
mode-mixity phase angle was increased to -25° >> -65°, the crack path was directly in the<br />
face/core interface. In the panels <strong>and</strong> the MMB specimens with H250 core the debond<br />
propagates directly in the interface. This may be explained by the higher fracture toughness <strong>of</strong><br />
the H250 core compared to H130 <strong>and</strong> PMI cores. Fibre bridging was observed after more than 4-<br />
5 mm crack growth in the MMB specimens <strong>and</strong> panels with H250 core. The similarity between<br />
the debond propagation paths in the MMB specimens <strong>and</strong> the panels refutes the role <strong>of</strong> the<br />
different propagation paths in the inaccuracy <strong>of</strong> the determined debond propagation loads.<br />
60