=πσ^2At the moment of fracture, G is equal to the critical energy-release rat e Gc, a function of the fracture
toughness. The value of Gc for a material can be determined via a relatively straightforward set of crack
experiments.
For a single-fracture mode, the stress-intensity factor and the energy-release rat e are related by:
=
′where G is the energy-release rate,
′=
−ν for plane strain, and ′= for plane stress. (E is thematerial Young’s modulus, and ν is the Poisson’s ratio.)
For more information, see VCCT Energy-Release Rat e Calculation (p. 356).
11.1.2.3. Stress-Intensity Factor
Limited to linear elastic material, the stress and strain fields ahead of the crack tip are expressed as:
σij= − ijθε= − θwhere K is the stress-intensity factor, r and θ are coordinates of a polar coordinate system (as shown in
Figure 11.2: Schematic of a Crack Tip (p. 342)). These equations apply to any of the three fracture modes.
Figure 11.2: Schematic of a Crack Tip
CrackyxrθFor a Mode I crack, the stress field is given as:
σ
πθ θ θ
= I
−
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