1996
DOI: 10.1007/bf00037233
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Modeling and simulation of crack propagation in mixed-modes interlaminar fracture specimens

Abstract: A study of mixed-mode crack propagation in bending-based interlaminar fracture specimens is here presented. A numerical scheme to simulate full crack propagation is proposed which makes use of interface laws relating interlaminar stresses to displacement discontinuities along the plane of crack propagation. The relation between interface laws and mixed-mode failure loci in terms of critical energies is discussed and clarified. Numerical simulations are presented and compared with analytical and experimental re… Show more

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Cited by 154 publications
(83 citation statements)
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“…These procedures, which may be considered to stem from the work of Hilleborg [9], include the 'cohesive zone model' [10; 11]. In relation to the simulation of delamination, the method has often been applied in conjunction with interface elements [12][13][14][15][16][17][18][19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%
“…These procedures, which may be considered to stem from the work of Hilleborg [9], include the 'cohesive zone model' [10; 11]. In relation to the simulation of delamination, the method has often been applied in conjunction with interface elements [12][13][14][15][16][17][18][19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%
“…It is thus recommend adjusting the shape of the CZM laws to conform to the behaviour of the thin material strip or interface they are simulating. Developed CZM include triangular [17], linear-parabolic [18], polynomial [19], exponential [20] and trapezoidal laws [21]. Thus, CZM can also be adapted to simulate ductile adhesive layers, whose behaviour can be approximated with trapezoidal laws [14].…”
Section: Introductionmentioning
confidence: 99%
“…It is worth recalling that also Alfano and Crisfield (2001) introduce a restriction to specialize the 2 damage parameters model of Crisfield and coworkers Mi et al (1998) to a 1 damage parameter model so as to achieve simultaneous complete debonding in mode I and II. Similarly, other authors (Allix and Corigliano, 1996;Corigliano, 1993) add this 'simultaneity' condition as a further constraint to the evolution equations. The second requirement for thermodynamic consistency is represented by the fulfillment of equation (28).…”
Section: Equivalent Displacement Functionmentioning
confidence: 99%