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NONLINEAR FRACTURE MECHANICS THE (非线性断裂力学)
NONLINEAR FRACTURE MECHANICS
THE COHESIVE CRACK MODEL
(Dugdale, D.S.: Yielding of steel sheets containing slits, J. Mechanics
Physics Solids 8 (1960), 100-104
Barenblatt, G.I.: The formation of equilibrium cracks during brittle fracture.
General ideas and hypotheses. Axially-symmetric cracks, J. Applied
Mathematics and Mechanics 23 (1959), 622-636.
Barenblatt, G.I.: The mathematical theory of equilibrium cracks in brittle
fracture, in H.L. Dryden and T. von Karman (eds.), Advanced in Applied
Mechanics, Academic Press, New York, 1962, pp. 55-129.)
ductile materials ⇒ Dugdale’s model
purely brittle materials ⇒ Barenblatt’s model
quasi brittle materials ⇒ Hillerborg’s Fictitious
(e.g. concrete) Crack Model
brittle matrix composites ⇒ Bridged crack model
quasi brittle matrix composites ⇒ Cohesive crack model
cohesive crack model 1
Dugdale’s Model for ductile fracture
Fracture of elasto-plastic materials
Assumptions:
- Mode I crack in an infinite sheet under uniform tensile
stress
- the material is ductile and the plastic deformations
localized in a thin zone coplanar with the crack
- the plastic zone is modeled through a fictitious crack (of
unknown length) and a uniform distribution of cohesive
tractions σP = yield stress
Length of the cohesive zone
The length of the cohesive zone aP is calculated by
imposing the condition of smooth closure of the crack faces:
KI KIσ + KIσ P 0
where: KIσ σ π (a + aP )
cohesive crack model 2
The SIF due to the plastic stresses is calculated using the
SIFs d
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