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Report - PEER - University of California, Berkeley

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espect to X has presumably been established, in principle one may select recordsfrom any values <strong>of</strong> X (Iervolino, 2004). In practice even in this case it is prudent touse records from the general magnitude regime <strong>of</strong> interest. In deciding which recordcharacteristics to mirror in the selection it is helpful to think in terms, primarily, <strong>of</strong>any systematic effects on spectral shape. Systematic spectral shape deviation fromthe appropriate range can effect linear response <strong>of</strong> MDOF systems and nonlinearresponse <strong>of</strong> even SDOF systems. Hence, for example, it is prudent to avoid selectingrecords from s<strong>of</strong>t soil sites or from records that may include directivity effects. If thesite should include such effects special efforts are necessary.Recent efforts (Baker, 2004b) have demonstrated that one such systematic effectis that <strong>of</strong> “epsilon”. Epsilon is the deviation <strong>of</strong> a record’s S a (at the structure’s firstmodeperiod, say) from that expected for the record’s specific values <strong>of</strong> X; in short itis the deviation or “residual” from the S a attenuation law (normalized by the “sigma”or standard error <strong>of</strong> the law.) High epsilon values are associated with peaks in therecord’s spectrum, and hence (for a fixed S a or IM level) with more benign nonlinearbehavior. (As the effective period <strong>of</strong> the structure lengthens it “falls <strong>of</strong>f the peak” andinto a less energetic portion <strong>of</strong> the frequency content.) But rare, high IM levels (orlow λ IM levels) that contribute most directly to rare MIDR levels are in turn associatedwith high values <strong>of</strong> epsilon (as evidenced in PSHA disaggregations for epsilon).Therefore when selecting records for analyses at these high IM levels one shouldconsider choosing them from among records that have comparable epsilon levels(e.g., 1 to 2), in order that they do have the right, non-smooth shape near the period <strong>of</strong>interest. This is one reason why selecting records with shapes close to that <strong>of</strong> theUHS (or artificially matching a record’s spectrum to the UHS) may bias the responseconservatively.Spectrum-matched or “spectrum-compatible” records have the advantage <strong>of</strong>reducing the dispersion in the response and hence <strong>of</strong> reducing the required samplesize. There is also evidence that they are unconservatively biased for large ductilitylevels (Carballo, 2000).Geophysically sound synthetics may be the only way we can obtain appropriaterecords for certain infrequently recorded cases, such as very near the source <strong>of</strong> largemagnitude events. The various empirically based schemes <strong>of</strong> record simulation (e.g.,from simple to evolutionary power spectral models, ARMA-based procedures, etc.)have the merit that one can produce from them large samples <strong>of</strong> nominally similar“earthquakes”. Care should be exercised to insure that their spectra are “roughenough” for accurate nonlinear analysis.2.6 Seeking Better IMs: Sufficiency and EfficiencyThe benefits <strong>of</strong> sufficient IMs are clearly a reduction in difficulty and reduction in thenumber <strong>of</strong> nonlinear analyses. The observation raises the subject <strong>of</strong> seeking stillbetter IMs, i.e., ones that might prove sufficient over a broader range <strong>of</strong> seismicconditions (i.e., regions <strong>of</strong> X ) and ones that might reduce the dispersion in response44

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