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Residual Strength and Fatigue Lifetime of ... - Solid Mechanics

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compared to the 65% efficiency obtained for the simulation <strong>of</strong> fatigue crack growth in s<strong>and</strong>wich<br />

beams in Chapter 4, the computational efficiency is here more than 33% higher. This is due to a<br />

somewhat unrealistic <strong>and</strong> arbitrary choice <strong>of</strong> da/dN vs. G relations in the simulations in Chapter<br />

4, where the da/dN vs. G relations were chosen so that the crack reaches the end <strong>of</strong> the<br />

specimens in hundreds <strong>of</strong> cycles to make the reference simulation <strong>of</strong> all individual cycles<br />

possible. The use <strong>of</strong> realistic da/dN vs. G relations here makes the crack growth significantly<br />

smaller in every cycle <strong>and</strong> provides room for more cycle jumps in the simulation.<br />

Table 5.3: Computational efficiency <strong>of</strong> the simulations with different control parameters.<br />

Control parameter<br />

qG=q<br />

Number <strong>of</strong> simulated cycles<br />

H45 specimen Saved cycles (%) H100 specimen Saved cycles (%)<br />

0.05 1104 98.896 1096 98.904<br />

0.10 548 99.452 557 99.443<br />

0.15 411 99.589 381 99.619<br />

0.20 312 99.688 323 99.677<br />

0.25 243 99.757 188 99.812<br />

5.3 <strong>Fatigue</strong> Crack Growth in the Face/Core Interface <strong>of</strong><br />

S<strong>and</strong>wich Panels<br />

In this section the 3D fatigue crack growth scheme developed in Chapter 4 is used to simulate<br />

fatigue crack growth in debonded s<strong>and</strong>wich panels with a circular debond at the centre. The<br />

simulation results will be compared with fatigue experiments at the end <strong>of</strong> this section.<br />

5.3.1 <strong>Fatigue</strong> Experiments on Debonded Panels<br />

Five s<strong>and</strong>wich panels with a circular face/core debond at the centre were manufactured for<br />

fatigue experiments. The panel face sheets consist <strong>of</strong> three layers <strong>of</strong> Devold AMT DBLT 850<br />

quadraxial glass fibre mats <strong>of</strong> a total thickness <strong>of</strong> 2 mm, each with a dry density <strong>of</strong> 850g/m 2 . The<br />

core materials are H45 Divinycell PVC foam with nominal densities <strong>of</strong> 45 kg/m 3 . The core thickness<br />

is 50 mm. The properties <strong>of</strong> the core materials, taken from the manufacturers’ data sheets (DIAB),<br />

<strong>and</strong> the face materials are given in Table 5.4. Figure 5.34 presents a drawing <strong>of</strong> the panels, including<br />

the dimensions, <strong>and</strong> an image showing one <strong>of</strong> the manufactured panels.<br />

114

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