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Report - PEER - University of California, Berkeley

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emain the same, the magnitude <strong>of</strong> sliding displacement is less for equipment withhigher µ and φ values.Probability <strong>of</strong> exceedenceProbability <strong>of</strong> exceedences1.00.80.60.40.2(a)DM = 5 cmµs= 0.3, φ = 0.5µs= 0.3, φ = 0.9µs= 0.7, φ = 0.5µs= 0.7, φ = 0.90.00.0 0.5 1.0 1.5 2.0 2.5Peak horizontal floor acceleration (g)1.00.80.60.40.2(b)DM = 10 cm0.00.0 0.5 1.0 1.5 2.0 2.5Peak horizontal floor acceleration (g)Probability <strong>of</strong> exceedenceProbability <strong>of</strong> exceedence1.00.80.60.40.2(c)DM = 30 cm/s0.00.0 0.5 1.0 1.5 2.0 2.5Peak horizontal floor acceleration (g)1.00.80.60.40.2(d)DM = 50 cm/s0.00.0 0.5 1.0 1.5 2.0 2.5Peak horizontal floor acceleration (g)Figure 3. Effect <strong>of</strong> µ andsφ on seismic fragility curves, considering differentDMs.4.2 Effect <strong>of</strong> Building Characteristics on the Fragility CurvesTo study the effect <strong>of</strong> the dynamic behavior <strong>of</strong> different building structures on thefragility curves, two additional 8-story building models are constructed. Thesebuildings, with a steel moment resisting frame (SMRF) construction; have beenpreviously considered by Santa-Ana and Miranda (2000). Both structures have thesame floor plan consisting <strong>of</strong> three bays in each direction. However, column andbeam details vary between the two buildings, such that one is relatively flexible,while the other is relatively stiff. The buildings have a uniform mass distribution anda non-uniform lateral stiffness distribution over their height. They were designedusing the lateral load distribution specified in the 1994 Uniform Building Code(ICBO, 1994), with member stiffness tuned to obtain fundamental periods <strong>of</strong>vibration for each structure representative <strong>of</strong> those obtained from earthquake records<strong>of</strong> instrumented existing SMRFs. The fundamental periods <strong>of</strong> vibration for these twostructures are T 1 = 1.92 and 1.19 seconds, for the flexible and stiff structures,respectively. In the following discussion, the nomenclature Steel-1 and Steel-2 is usedto refer to the flexible and stiff structure, respectively.Numerical models <strong>of</strong> these structures were developed in OpenSees (2003) forthese structures, considering a representative 2D frame <strong>of</strong> the building in thetransverse direction [Figures 4(b) and (c)]. Both geometric nonlinearity and materialnonlinearity are accounted for the model. A lumped mass model is used, with thebuildings assumed fixed at the ground surface. Two percent Rayleigh massproportional damping is used and kinematic material hardening is assumed.204

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