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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These numerical <strong>and</strong> experimental studies provide a better underst<strong>and</strong>ing <strong>of</strong> the behaviour <strong>of</strong><br />
debond damaged s<strong>and</strong>wich composites under static or fatigue loading. Moreover, they develop<br />
reliable analysis tools for assessing the damage tolerance <strong>and</strong> fatigue lifetime <strong>of</strong> debonded<br />
s<strong>and</strong>wich composites.<br />
Since Linear Elastic Fracture <strong>Mechanics</strong> (LEFM) for the interfaces is the main theoretical<br />
foundation <strong>of</strong> this thesis, it will be presented in the next section <strong>of</strong> the Introduction. Finally, a<br />
brief history <strong>of</strong> fatigue analysis in s<strong>and</strong>wich composites will be presented in the last section <strong>of</strong><br />
the Introduction.<br />
1.3 Linear Elastic Fracture <strong>Mechanics</strong><br />
Griffith in 1920 established the foundations <strong>of</strong> fracture mechanics. He applied a stress analysis <strong>of</strong><br />
an elliptical hole from Inglis (1913) to the unstable crack propagation problem. Based on the<br />
principle <strong>of</strong> energy conservation <strong>of</strong> thermodynamics, Griffith proposed the energy balance<br />
concept for fracture. According to Griffith’s theory, a crack may be formed or propagate if the<br />
potential energy change provided by strain energy <strong>and</strong> external forces, resulting from crack<br />
growth, is enough to overcome the surface energy <strong>and</strong> generate new surfaces. In 1948 Irwin<br />
extended Griffith’s concept to metals by including plastic energy dissipation at the crack tip. In<br />
1956 Irwin proposed the Griffith energy or energy release rate G as a measure <strong>of</strong> available<br />
energy for crack growth as<br />
<br />
<br />
where is the potential energy <strong>and</strong> dA is the crack area increment. According to Equation (1.1)<br />
the critical energy release rate Gc or fracture toughness can be defined as<br />
<br />
<br />
where Ws is the required energy for creation <strong>of</strong> new surfaces.<br />
Generally, a crack may experience three types <strong>of</strong> loading, see Figure 1.3. Mode I loading where<br />
the applied load tends to open the crack, mode II loading where the in-plane shear loading tends<br />
to slide one crack face against the other <strong>and</strong> mode III corresponding to the out-<strong>of</strong>-plane shear <strong>and</strong><br />
sliding <strong>of</strong> the crack flanks. A crack may be loaded in any <strong>of</strong> these three modes or in a mixedmode<br />
combination <strong>of</strong> them. In 2D modelling <strong>of</strong> a crack problem, only the first two modes are<br />
typically used.<br />
5<br />
(1.1)<br />
(1.2)