Report - PEER - University of California, Berkeley
Report - PEER - University of California, Berkeley Report - PEER - University of California, Berkeley
Pinto et al., 2004). The probability of being in a particular damage band may then beobtained from the difference between the bordering limit state exceedanceprobabilities.3.1 Probabilistic Treatment of the DemandThe cumulative distribution function of the displacement demand can be found usingthe median displacement demand values and their associated logarithmic standarddeviation at each period. The cumulative distribution function can be used to obtainthe probability that the displacement demand exceeds a certain value (x), given aresponse period (T Lsi ) for a given magnitude-distance scenario.The displacement demand spectrum that might be used in a loss estimation studycould take the form of a code spectrum or else a uniform hazard spectrum derivedfrom PSHA for one or more annual frequencies of exceedance. Both of these optionshave drawbacks in being obtained from PSHA wherein the contributions from allrelevant sources of seismicity are combined into a single rate of occurrence for eachlevel of a particular ground-motion parameter. The consequence is that if the hazard iscalculated in terms of a range of parameters, such as spectral ordinates at severalperiods, the resulting spectrum will sometimes not be compatible with any physicallyfeasible earthquake scenario. Furthermore, if additional ground-motion parameters,such as duration of shaking, are to be incorporated – as they are in HAZUS (FEMA,1999), in the definition of the inelastic demand spectrum – then it is more rational notto combine all sources of seismicity into a single response spectrum but rather to treatindividual earthquakes separately, notwithstanding the computational penalty that thisentails. Another advantage of using multiple earthquake scenarios as opposed toPSHA is the facility of being able to disaggregate the losses and identify theearthquake events contributing most significantly to the damage.The approach recommended therefore is to use multiple earthquake scenarios,each with an annual frequency of occurrence determined from recurrencerelationships. For each triggered scenario, the resulting spectra are found from aground-motion prediction equation. In this way, the aleatory uncertainty, asrepresented by the standard deviation of the lognormal residuals, can be directlyaccounted for in each spectrum. The cumulative distribution function of thedisplacement demand can then be compared with the joint probability densityfunctions of displacement capacity and period (Section 3.2), and the annualprobability of failure for a class of buildings can be found by integrating the failureprobabilities for all the earthquake scenarios (see Crowley et al., 2004).3.2 Probabilistic Treatment of the CapacityAs has been presented previously, the limit state displacement capacity (∆ Lsi ) of eachbuilding class can be defined as a function of the fundamental period (T Lsi ), thegeometrical properties of the building, and the mechanical properties of the180
construction materials. Similarly, the limit state period (T Lsi ) of each building classcan be defined as a function of the height (or number of storeys), the geometricalproperties of the building, and the mechanical properties of the construction materials.The uncertainty in ∆ Lsi and in T Lsi is accounted for by constructing a vector ofparameters that collects their mean values and standard deviations. By assigningprobability distributions to each parameter, FORM can be used to find both thecumulative distribution function (CDF) of the limit state displacement capacity,conditioned to a period, and the CDF of the limit state period, which are thencombined to create the joint probability density function of capacity.3.2.1 Probabilistic Modelling of Geometrical PropertiesA given building class within a selected urban area may comprise a large number ofstructures that present the same number of storeys and failure mode, but that featurevarying geometrical properties (e.g., beam height, beam length, column depth,column/storey height), due to the diverse architectural and loading constraints thatdrove their original design and construction. Since such variability does affect in asignificant manner the results of loss assessment studies (see Glaister and Pinho,2003), it is duly accounted for in the current method by means of the probabilisticmodelling described below.Clearly, one could argue that by carrying out a detailed inspection of the buildingstock, such variability could be significantly reduced (in the limit, if all buildingswere to be examined, it could be wholly eliminated), however at a prohibitive cost interms of necessary field surveys and modelling requirements (vulnerability wouldthen be effectively assessed on a case-by-case basis). This epistemic component ofthe geometrical variability of reinforced concrete members has been modelled in thepresent work by means of normal or log-normal probability distribution functions,derived from European building stock data, as described in Crowley et al. (2004).3.2.2 Probabilistic Modelling of Reinforcing Bar Yield StrainMirza and MacGregor (1979) have suggested that once a probabilistic distribution foryield strength has been found, it can be divided by a deterministic value of themodulus of elasticity, which features a very low coefficient of variation, to producethe distribution of the yield strains. These two researchers have also concluded,through a series of experimental parametric studies, that a normal distribution wouldaccurately represent the variability of reinforcement bars’ yield strength, in thevicinity of the mean, whilst a beta distribution correlated well over the whole range ofdata. The coefficient of variation in the yield strength was found to be between 8% -12% when data were taken from different bar sizes from many sources. Morerecently, the Probabilistic Model Code (JCSS, 2001) has also suggested that a normaldistribution can be adopted to model the yield strength of steel. Therefore, a normaldistribution for the steel yield strength (and subsequently yield strain) has beenadopted in the current work.181
- Page 146 and 147: for these flexible nonstructural co
- Page 148 and 149: spectra is several times larger tha
- Page 150 and 151: The variability is associated with
- Page 152 and 153: functions for a wide variety of non
- Page 154 and 155: SIMPLIFIED PBEE TO ESTIMATE ECONOMI
- Page 156 and 157: One can show (Porter et al. 2004) t
- Page 158 and 159: ( )FDM| EDP= xdm = 1 −FRdm , + 1,
- Page 160 and 161: 1. Facility definition. Same as in
- Page 162 and 163: Table 1. Approximation of seismic r
- Page 164 and 165: The EAL values shown in Figure 3 mi
- Page 166 and 167: ASSESSMENT OF SEISMIC PERFORMANCE I
- Page 168 and 169: where e -λτ is the discounted fac
- Page 170 and 171: IDR 3[rad]σPFAIDR34(g)σ PFA4media
- Page 172 and 173: Figure 3a, shows an example of frag
- Page 174 and 175: P(C LVCC i |IM )1.00.80.60.40.20.00
- Page 176 and 177: E [ L T | IM ]$ 10 M$ 8 M$ 6 M$ 4 M
- Page 178 and 179: SEISMIC RESILIENCE OF COMMUNITIES
- Page 180 and 181: 2. RESILIENCE CONCEPTSResilience fo
- Page 182 and 183: quantification tools could be used
- Page 184 and 185: structure remains elastic. This is
- Page 186 and 187: of Figure 7a will be used. It is as
- Page 188 and 189: Nigg, J. M. (1998). Empirical findi
- Page 190 and 191: acceleration with a 475-year return
- Page 192 and 193: limit states, the suggestions given
- Page 194 and 195: ∆NSLsi= SϑH(5)iTFor column-sway
- Page 198 and 199: The main difficulty in assigning a
- Page 200 and 201: Crowley, H., R. Pinho, and J. J. Bo
- Page 202 and 203: analytical models generally have si
- Page 204 and 205: Figure 2. Structure of the response
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- Page 208 and 209: 4. DERIVATION OF THE VULNERABILITY
- Page 210 and 211: 5. CONCLUSIONSDerivation of vulnera
- Page 212 and 213: REFERENCESAbrams, D. P., A. S. Elna
- Page 214 and 215: In general, these types of bench-mo
- Page 216 and 217: where & x&(t ) = acceleration at th
- Page 218 and 219: science building. The lateral load-
- Page 220 and 221: emain the same, the magnitude of sl
- Page 222 and 223: of sliding thresholds, are desirabl
- Page 224 and 225: Retrofit of Nonstructural Component
- Page 226 and 227: was developed to accommodate these
- Page 228 and 229: tested by Meinheit and Jirsa are us
- Page 230 and 231: where D is the maximum drift and N
- Page 232 and 233: in predicting damage as well as rep
- Page 234 and 235: 4.2.2 Modeling the Data Using Stand
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- Page 238 and 239: • The influence on the dynamic re
- Page 240 and 241: deviations σ and correlation coeff
- Page 242 and 243: The first three modes of vibration
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construction materials. Similarly, the limit state period (T Lsi ) <strong>of</strong> each building classcan be defined as a function <strong>of</strong> the height (or number <strong>of</strong> storeys), the geometricalproperties <strong>of</strong> the building, and the mechanical properties <strong>of</strong> the construction materials.The uncertainty in ∆ Lsi and in T Lsi is accounted for by constructing a vector <strong>of</strong>parameters that collects their mean values and standard deviations. By assigningprobability distributions to each parameter, FORM can be used to find both thecumulative distribution function (CDF) <strong>of</strong> the limit state displacement capacity,conditioned to a period, and the CDF <strong>of</strong> the limit state period, which are thencombined to create the joint probability density function <strong>of</strong> capacity.3.2.1 Probabilistic Modelling <strong>of</strong> Geometrical PropertiesA given building class within a selected urban area may comprise a large number <strong>of</strong>structures that present the same number <strong>of</strong> storeys and failure mode, but that featurevarying geometrical properties (e.g., beam height, beam length, column depth,column/storey height), due to the diverse architectural and loading constraints thatdrove their original design and construction. Since such variability does affect in asignificant manner the results <strong>of</strong> loss assessment studies (see Glaister and Pinho,2003), it is duly accounted for in the current method by means <strong>of</strong> the probabilisticmodelling described below.Clearly, one could argue that by carrying out a detailed inspection <strong>of</strong> the buildingstock, such variability could be significantly reduced (in the limit, if all buildingswere to be examined, it could be wholly eliminated), however at a prohibitive cost interms <strong>of</strong> necessary field surveys and modelling requirements (vulnerability wouldthen be effectively assessed on a case-by-case basis). This epistemic component <strong>of</strong>the geometrical variability <strong>of</strong> reinforced concrete members has been modelled in thepresent work by means <strong>of</strong> normal or log-normal probability distribution functions,derived from European building stock data, as described in Crowley et al. (2004).3.2.2 Probabilistic Modelling <strong>of</strong> Reinforcing Bar Yield StrainMirza and MacGregor (1979) have suggested that once a probabilistic distribution foryield strength has been found, it can be divided by a deterministic value <strong>of</strong> themodulus <strong>of</strong> elasticity, which features a very low coefficient <strong>of</strong> variation, to producethe distribution <strong>of</strong> the yield strains. These two researchers have also concluded,through a series <strong>of</strong> experimental parametric studies, that a normal distribution wouldaccurately represent the variability <strong>of</strong> reinforcement bars’ yield strength, in thevicinity <strong>of</strong> the mean, whilst a beta distribution correlated well over the whole range <strong>of</strong>data. The coefficient <strong>of</strong> variation in the yield strength was found to be between 8% -12% when data were taken from different bar sizes from many sources. Morerecently, the Probabilistic Model Code (JCSS, 2001) has also suggested that a normaldistribution can be adopted to model the yield strength <strong>of</strong> steel. Therefore, a normaldistribution for the steel yield strength (and subsequently yield strain) has beenadopted in the current work.181