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

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high growth rate <strong>of</strong> G (see Figure 4.7), but approaching the end <strong>of</strong> 500 cycles with decreasing<br />

G, crack increment becomes smaller. The simulation with qG=q=0.05 follows the reference<br />

simulation with good agreement, but the simulation with qG=q=0.2 shows again less accuracy.<br />

(a)<br />

(b)<br />

Figure 4.8: Crack length vs. number <strong>of</strong> cycles for control parameters (a) qG=q = 0.05 <strong>and</strong> (b)<br />

qG=q = 0.2.<br />

Figure 4.9 presents the phase angle vs. number <strong>of</strong> cycles. The same conclusion may be drawn<br />

upon the accuracy <strong>of</strong> the simulation using the cycle jump method <strong>and</strong> the two control parameters<br />

qG=q=0.05 <strong>and</strong> qG=q=0.2.<br />

(a)<br />

(b)<br />

Figure 4.9: (a) Mode- mixity phase angle vs. number <strong>of</strong> cycles for the reference analysis <strong>and</strong><br />

the analyses with qG=q=0.05 <strong>and</strong> qG=q=0.2 as control parameters.<br />

To measure the computational efficiency <strong>of</strong> the cycle jump method for analyses with different<br />

control parameters, the ratio R is introduced:<br />

N jump<br />

R (4.11)<br />

N<br />

ref<br />

where Njump is the number <strong>of</strong> jumped cycles <strong>and</strong> Nref is the total number <strong>of</strong> cycles in the reference<br />

72

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