By Z. Tonkovic, M. H. Aliabadi
Advances in Fracture and harm Mechanics X cointains chosen, peer reviewed papers submitted on the tenth foreign convention on Fracture and harm Mechanics which came about in Dubrovnik.
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Extra info for Advances in Fracture and Damage Mechanics X: Selected, Peer Reviewed Papers from the 10th International Conference on Fracture and Damage Mechanics ... Dubrovnik, C
6) VGM and SMCS already have a defined shape for fracture locus, instead BW accordingly with  have a more complex form. BW fracture locus has to be partially arbitrary defined. Thus it has been chosen a hyperbola with equation: ε pfailure (η ) = C 1 +η 3 . 2. 2. 0377 All the calibrated fracture locus can be seen in Fig. 3a. It’s important to remark that each curve is related at a different criterion and this means that their interpretation is different. This explains why there is so much difference among them.
Asadikouhanjani, K. H Ayed: Fracture Analysis of a First Stage Turbine Blade, Proceedings of ASME Turbo Expo 2010: Power for Land, Sea and Air.  B. N. J. Persson, E. Tosatti: Physics of sliding friction, chapter I, Kluwer Academic Publishers (1996).  W. Hoffelner: METALL TRANS A Vol. 13A (1982), p. 1245. htm. 21 Fully Reversed Uniaxial Tension-Compression High Cycle Fatigue Behaviour of Shot-peened Steels A. M. Mirzazadeh1,b Department of Mechanical and Mechatronics Engineering, University of Waterloo, 200 University Ave.
In classical lattice models, the material is represented by a set of discrete elements inter-connected by springs. The use of a combination of simple constitutive models with a material structure incorporated from the mesolevel [1,2], or alternatively of material parameters whose randomness somehow mimics this material structure [3,4], makes such models powerful tools able to model quasibrittle structural response. It is an alternative to the relatively complex constitutive laws applied in classical continuum mechanics-based models.