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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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4.3. Elasto-plastic joint/interface model with isotropic linear softeningFigure 4.3: Schematic components of pull-out analysis for the analytical solution.matrix interface. Accor<strong>di</strong>ng to the plasticity model described in section 4.3, the contactlaw (τ − s) presents a bilinear form, featuring an initial linear ascen<strong>di</strong>ng branch, withthe k E initial slope, followed, when the elastic limit τ y,0 is reached, by a linear softeningbranch whose slope is now defined as k S = k E(1 − k Ek E +k H). The model is completedconsidering an ultimate slip, s u , at which the bond transferred stress is considered null.The full analytical solution is applied to a single fiber, as schematized in Figure 4.3.Based on the assumption that the fiber <strong>di</strong>ameter d f and the local bond-slip relationshipkeep unchanged throughout the fiber bond length, l emb , the following infini<strong>tesi</strong>malequilibrium con<strong>di</strong>tion can be formulateddσ f [z]d z= − 4τ[z]d f(4.7)where τ[z] is the shear stress transferred at the interface and σ f [z] the axial steel stress.Assuming that bond failure occurs for fiber stresses lower than the correspon<strong>di</strong>ng yieldlimit (as generally observed in experimental investigations), the following constitutivelaws to model both the mechanical response of fiber and the interface adherences,respectively, can be writtenσ f [z] = E fd s[z]d z(4.8)73

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