4.7 Article

Cohesive-zone models and singularities at corners and cracks in homogeneous materials

Journal

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jmps.2022.105159

Keywords

Corners; Mixed-mode fracture; Cohesive-zones; Singularities

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The stress singularities at corners of elastic bodies are not strong enough to cause fracture, unless there is a crack. This study re-examines these elastic stresses using cohesive-zone models and presents a framework to understand fracture at corners. It shows that the cohesive length, xi, plays a crucial role in allowing fracture (and slip) at a corner, and how stress-intensity factor and phase angle reduce to linear-elastic fracture mechanics in the case of a crack. The study also reveals that the normal and shear deformations across the interface at a corner are generally coupled, leading to complex behavior.
The stress singularities at corners in elastic bodies are not strong enough to provide a driving force for fracture, except in the limit of a crack. Here, we re-examine these elastic stresses from the perspective of cohesive-zone models. We present a general framework to understand fracture at corners, and define the magnitude of a stress-intensity factor and its phase angle, showing how these reduce to the familiar concepts of linear-elastic fracture mechanics (LEFM), in the special case of a crack. We discuss how the cohesive length, xi , which is inherent to cohesivezone models, is responsible for permitting fracture (and slip) at a corner. The work done against the tractions at a corner scales with xi(1-2n). and xi(1-2n), where n and m are the strengths of the two elastic stress singularities. Therefore, except in the case of a crack, for which n = m = 0.5 and the dependency on the cohesive length disappears, the work goes to zero in the classical elasticity limit of xi = 0, and neither fracture nor slip can occur. Using simple, uncoupled traction-separation laws, we show that the normal and shear deformations across the interface at a corner are generally coupled, despite the lack of explicit coupling in the laws. The crack-tip phase angle is shifted from the applied phase angle, and the properties of each traction-separation law affects the deformation in the other mode. These features lead to a very rich behavior that would be further complicated by consideration of more complex laws.

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