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tesi A. Caggiano.pdf - EleA@UniSA - Università degli Studi di Salerno

tesi A. Caggiano.pdf - EleA@UniSA - Università degli Studi di Salerno

tesi A. Caggiano.pdf - EleA@UniSA - Università degli Studi di Salerno

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3.3. Fracture energy-based model for plain mortar/concrete interfacewhere ˙u = [ ˙u, ˙v] t is the rate of the relative joint <strong>di</strong>splacement vector, decompose<strong>di</strong>nto the elastic and plastic components, ˙u el and ˙u cr , respectively. C defines a fullyuncoupled normal/tangential elastic stiffness matrixC =()k N 0(3.13)while ṫ i = [ ˙σ N , ˙σ T ] t is the incremental stress vector defined in the interface coor<strong>di</strong>nates,being σ N and σ T the normal and shear components, respectively.σ Τc tan (φ )tan (β )χ− σ <strong>di</strong>l− σ Ν-150Mohr-Coulomb CriterionPlastic Potential-250Cracking SurfaceMo<strong>di</strong>fied flow ruleFigure 3.6: Failure hyperbola by Carol et al. [1997], Mohr-Coulomb surface, plastic potentialand the mo<strong>di</strong>fied flow rule accor<strong>di</strong>ng to Eq. (3.19) of the interface model.The vector of the plastic <strong>di</strong>splacement rate, accor<strong>di</strong>ng to a non-associated flow rule, isdefined as˙u cr = ˙λm (3.14)where ˙λ is the non-negative plastic multiplier derived by means of the classical Kuhn-Tucker loa<strong>di</strong>ng/unloa<strong>di</strong>ng and consistency con<strong>di</strong>tions which take the following form˙λ ≥ 0, f ≤ 0, ˙λ · f = 0 Kuhn − Tuckerf ˙ = 0Consistency(3.15)where f = f [σ N ,σ T ] defines the yield con<strong>di</strong>tion of the model on the bases of thefollowing three-parameter formulation (outlining the hyperbola represented in Figure51

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