Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Residual Strength and Fatigue Lifetime of ... - Solid Mechanics
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Figure 1.8: Typical fatigue crack growth rate vs. K diagram.<br />
The crack growth rate diagram is divided into an initiation phase (I), a stable crack growth phase<br />
(II) <strong>and</strong> an unstable crack growth phase (III), as shown in Figure 1.8. The initial phase includes<br />
non-continuous fracture processes with a very low crack growth rate. The stress intensity factor<br />
range in this phase approaches the fatigue crack growth threshold, Kth. The linear intermediate<br />
phase is the most interesting phase due to the linear relation between the logarithm <strong>of</strong> the crack<br />
propagation rate <strong>and</strong> the logarithm <strong>of</strong> the stress intensity factor. This phase covers a large range<br />
<strong>of</strong> stress intensity factors <strong>and</strong> crack propagation in this phase is generally more stable than in the<br />
two other phases. The linear phase <strong>of</strong> the diagram, also named the Paris regime, can be written as<br />
<br />
<br />
where m is the slope <strong>of</strong> the linear phase <strong>and</strong> c is the crack growth rate for K=1.<br />
11<br />
(1.20)<br />
In phase III the crack grows fast <strong>and</strong> in an unstable manner. The effect <strong>of</strong> the loading ratio,<br />
R=Fmin/Fmax, on the crack growth rate is shown in Figure 1.8. It is seen for a given crack growth<br />
rate that the K value increases with increased loading ratio. The influence <strong>of</strong> the loading ratio is<br />
due to the fact that the crack growth is mainly determined by the maximum stress intensity factor<br />
value for each fatigue cycle, Kmax, <strong>and</strong> its proximity to the fracture toughness <strong>of</strong> the material, Kc.<br />
In homogeneous materials due to the fact that the crack only experiences opening mode I<br />
loading, the crack growth rate diagram is unique. On the contrary, in an interface due to the<br />
existence <strong>of</strong> mixed-mode loading at the crack tip <strong>and</strong> the resistance <strong>of</strong> other layers toward<br />
kinking <strong>of</strong> the crack, different crack growth rate relations exist for different mode-mixities.