Issue 35

P. Bernardi et al, Frattura ed Integrità Strutturale, 35 (2016) 98-107; DOI: 10.3221/IGF-ESIS.35.12 106 loads, in terms of crack distribution and widths. Some of the obtained results have been reported in Fig. 6 (for brevity, only for specimen BN50 [18]). As can be seen, crack patterns are reasonably well described during the entire loading history, highlighting that the proposed model can represent a powerful tool in the analysis of RC structures also at serviceability conditions, where crack control represents one of the fundamental issues to be checked. For the analyzed beam, the first numerical flexural crack occurred at approximately the same loading level registered during the experimental test. As proved by both numerical and experimental results, this first crack has been followed by the appearance of subsequent flexural cracks, until the attainment of the last loading stage, when a significant shear diagonal crack developed as extension of existing cracks. w f-max = 0.10 mm w f-max = 0.21 mm w f-max = 0.15 mm w f-max = 0.37 mm w f-max = 0.20 mm w f-max = 0.41 mm w f-max = 0.05 mm w f-max = 0.05 mm w f-max = 0.10 mm w f-max = 0.30 mm w f-max = 0.20 mm w f-max = 0.41 mm LS1 LS3 LS5 LS2 LS4 LS6 BN50 LS1 → P=80 kN LS2 → P=100 kN LS3 → P=150 kN LS4 → P=180 kN LS5 → P=220 kN LS6 → P=250 kN LSF → Failure → P=260 kN w f-max = 0.20 mm w f-max = 0.43 mm LSF w [mm] Figure 6 : Numerical (left side) vs. experimental (right side, [18]) crack patterns and crack widths at different loading stages for specimen BN50. C ONCLUSIONS n this paper, a constitutive non-linear model for the analysis of reinforced concrete structures, named 2D-PARC, has been modified so as to improve its computational efficiency, while maintaining its capability of providing correct predictions of the structural behavior. To this aim, the constitutive relation originally adopted in 2D-PARC for the modeling of concrete, both before and after cracking, has been properly substituted by implementing the one proposed by Ottosen, which is based on non-linear elasticity and is characterized by a high numerical feasibility. The accuracy of the proposed formulation has been tested through comparisons with experimental results on RC beams without stirrups failing in shear, which represent a quite difficult case study, particularly when modelled through two-dimensional membrane analysis. Based on the obtained results, it has been generally proved that 2D-PARC model is able to provide accurate predictions of strength, load-deformation response and failure mode. Moreover, also crack pattern evolution, both in terms of crack distribution into the considered element and in terms of maximum crack width, can be satisfactorily evaluated. Finally, it can be pointed out that the modular structure of 2D-PARC model makes it an attractive and versatile alternative approach for the analysis of RC structures, since the representation of each single resistant contribution can be easily changed when more refined and/or efficient constitutive relations become available. I