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Simplified models/procedures for estimation of ... - ELSA - Europa

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24concrete struts can <strong>for</strong>m with the member axis an angle θ that can vary up to a value <strong>of</strong> 45°. Themethod recognises that due to shear mechanisms different from those considered by the Ritter–Mörsch truss model, the compressive stresses in the member web may have an inclination lowerthan 45°. According to this model the shear resistance <strong>of</strong> a member may be reached either <strong>for</strong>yielding <strong>of</strong> the stirrups:AvV = ⋅dv⋅ fvy⋅cotθ (8.4)sor <strong>for</strong> crushing <strong>of</strong> the concrete web struts:ν ′ ( θ θ)V = b⋅d ⋅ ⋅ f / cot + tan (8.5)vcwhere ν is the strength reduction factor <strong>for</strong> concrete cracked in shear and is computed as afunction <strong>of</strong> the compressive stress f’ c derived from cylinder tests:⎛ f ′ ⎞ν = 0.6⋅⎜1−c⎟ (f ’ c in MPa) (8.6)⎝ 250 ⎠Equation (8.6) accounts <strong>for</strong> the lower compression resistance <strong>of</strong> the concrete <strong>for</strong>ming the strutswith respect to the compression resistance derived from standard cylinder tests. This reduction inresistance is due to the high tensile strains that exist in the struts normal to the direction <strong>of</strong> thestruts and to the effects <strong>of</strong> the stirrups crossing the struts.For a given amount <strong>of</strong> transverse rein<strong>for</strong>cement the maximum shear resistance is attained whenthe yielding <strong>of</strong> the shear rein<strong>for</strong>cement and the crushing <strong>of</strong> the web concrete struts are reachedsimultaneously. This assumption leads to the following condition <strong>for</strong> angle θ:1−ωvcot θ = (8.7)ωvWith the mechanical percentage <strong>of</strong> web rein<strong>for</strong>cement ω v equal to:Av⋅ fvyωv=s⋅b⋅ν⋅ f ′cConsidering the values <strong>of</strong> θ given by Equation (8.7), the shear strength may be expressed as afunction <strong>of</strong> the amount <strong>of</strong> shear rein<strong>for</strong>cement, and may be plotted in a dimensionless <strong>for</strong>mat asshown in Fig. 2.1, indicating that larger shear capacities are obtained with respect to the Ritter –Mörsch truss model, which assumes a strut inclination <strong>of</strong> θ equal to 45°.The norm prEN 1992-1 [CEN, 2003] suggests to use as shear resistance <strong>of</strong> a member the lowestvalue resulting from Equations (8.4) and (8.5) <strong>for</strong> a given amount <strong>of</strong> shear rein<strong>for</strong>cement and <strong>for</strong>a given value <strong>of</strong> θ. For members subjected to axial compressive <strong>for</strong>ces, the same code suggests tomultiply the value given by Equation (8.5) by a factor α c ranging between 0 and 1.25 (see Fig.2.2), which depends on the mean compressive stress σ p acting on the section <strong>of</strong> the member.prEN 1992-1 [CEN, 2003] does not consider any distinction between the loads inducing thecompressive stresses, which may be either external (i.e., gravity loads) or due to prestressing orpostensioning. It should be noted that prEN 1992-1 [CEN, 2003] does not give any indication onthe effects on shear resistance associated to loads inducing tensile stresses on the section.Both <strong>of</strong> the approaches presented in the previous paragraphs (e.g., concrete contribution methodas given by Equation (8.1) and the variable angle truss model) are insensitive to the magnitudeand consequences <strong>of</strong> the member de<strong>for</strong>mations. Mechanisms such as tension stiffening,(8.8)

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