Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
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4.5 Conclusion<br />
A cycle jump method for accelerated simulation <strong>of</strong> fatigue crack growth in a bimaterial interface<br />
was presented in this chapter. The proposed method is based on finite element analysis for a set<br />
<strong>of</strong> cycles to establish a trend line, extrapolating the trend line which spans many cycles, <strong>and</strong> use<br />
the extrapolated state as an initial state for additional finite element simulations. Two finite<br />
element routines for accelerated fatigue crack growth simulation were developed. The first<br />
routine is suitable for 2D crack growth <strong>and</strong> the second is applicable to any 3D fatigue crack<br />
growth simulation with an arbitrary crack front shape. To assess the computational efficiency<br />
<strong>and</strong> accuracy <strong>of</strong> the developed finite element routines, they were used to simulate face/core<br />
interface fatigue crack growth in a s<strong>and</strong>wich beam (2D) <strong>and</strong> a s<strong>and</strong>wich panel (3D). The results<br />
were compared with a reference analysis simulating all individual cycles.<br />
By application <strong>of</strong> the cycle jump method, fatigue crack growth in the interface <strong>of</strong> a s<strong>and</strong>wich<br />
beam was simulated for 500 cycles as a numerical example. The computational efficiency <strong>and</strong><br />
accuracy <strong>of</strong> the cycle jump method was discussed <strong>and</strong> verified based on the three parameters:<br />
crack length, difference between maximum <strong>and</strong> minimum energy release rate in a cycle (G) <strong>and</strong><br />
mode-mixity phase angle against the reference analysis. The effect <strong>of</strong> the control parameters<br />
governing the implementation <strong>of</strong> the cycle jump method on the computational efficiency <strong>and</strong><br />
accuracy was studied. The results suggest that the computational efficiency <strong>of</strong> the simulations<br />
increases considerably with increasing the control parameters. However, the accuracy <strong>of</strong> the<br />
simulations decreases for crack length, G <strong>and</strong> mode-mixity phase angle determination. For the<br />
control parameters qG=q=0.05 the cycle jump method requires 175 cycles to simulate 500<br />
cycles, resulting in a 65% reduction in computational time with reasonably good accuracy<br />
(around 1% error).<br />
The second routine (3D) was used to simulate fatigue debond propagation in s<strong>and</strong>wich panels<br />
with an elliptical face/core debond at the centre <strong>of</strong> the panels. To make the simulation suitable<br />
for practical applications <strong>and</strong> due to lack <strong>of</strong> experimental methods for characterization <strong>of</strong> the<br />
effect <strong>of</strong> the mode III energy release rate, GIII, on the crack growth rate, only mode I <strong>and</strong> II<br />
components <strong>of</strong> the strain energy release rate were used in the crack growth routine. However, to<br />
analyse the effect <strong>of</strong> mode III loading at the crack tip, the mode III strain energy release rate was<br />
determined along the debond front. It was shown that the mode III crack tip loading is<br />
considerable close to the longer radius <strong>of</strong> the ellipse for an elliptical debond with large a/b radius<br />
ratios, which implies the importance <strong>of</strong> the development <strong>of</strong> new experimental methods for<br />
characterisation <strong>of</strong> the effect <strong>of</strong> mode III loading at the crack tip on the crack growth rate in such<br />
debond geometries.<br />
To examine the accuracy <strong>and</strong> computational efficiency <strong>of</strong> the developed 3D cycle jump method,<br />
a reference simulation, simulating all individual cycles <strong>and</strong> simulations based on the cycle jump<br />
method with different control parameters were conducted. It was shown that with good accuracy<br />
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