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Peak displacement (m)<br />

84, 50, 16 percentiles<br />

1.2<br />

0.8<br />

0.4<br />

LBin 1a<br />

LBin 1b<br />

Lyield displ.<br />

0<br />

0 0.4 0.8 1.2 1.6 2<br />

Period (sec)<br />

β<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 0.4 0.8 1.2 1.6 2<br />

Period (sec)<br />

a. Peak displ., Fy<br />

= 40% W<br />

b. β , Fy<br />

= 40% W<br />

1.2<br />

0.8<br />

Peak displacement (m)<br />

84 , 5 0, 16 p erce ntile s<br />

0.8<br />

0.4<br />

0<br />

0 0.4 0.8 1.2 1.6 2<br />

Period (sec)<br />

β<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 0.4 0.8 1.2 1.6 2<br />

Period (sec)<br />

c. Peak displ., Fy<br />

= 20% W<br />

d. β , Fy<br />

= 20% W<br />

1.2<br />

0.8<br />

Peak displacement (m)<br />

84, 50, 16 percentiles<br />

0.8<br />

0.4<br />

0<br />

2 2.4 2.8 3.2 3.6 4<br />

Period (sec)<br />

β<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

2 2.4 2.8 3.2 3.6 4<br />

Period (sec)<br />

e. Peak displ., F = 6% W<br />

f. β , F = 6% W<br />

y<br />

Figure 22 Median, 84th and 16th percentiles and β of peak displacement response for Bins 1a and 1b<br />

Method 2: Spectrum-Matching Method<br />

Spectrally matched ground motions are often used to compute seismic demands in structural framing systems.<br />

To judge the utility of spectrum-matched ground motions for predicting the response of nonlinear SDOF<br />

framing systems (such as base-isolated structures), the NF seed motions of Table 1 were modified to match the<br />

median spectrum of Bin 1a using the computer code RSPMATCH (Abrahamson 1998, Hancock et al. 2006).<br />

<strong>The</strong> bin of 50 spectrally matched motions is labeled as Bin 1b. <strong>The</strong> 16th, 50th and 84th percentiles of elastic<br />

spectral acceleration for Bin 1b are shown in Figure 20a. <strong>The</strong> median spectral accelerations for Bins 1a and 1b<br />

are virtually identical. Figure 20b presents the dispersion in the spectral accelerations for the two bins of ground<br />

motions. <strong>The</strong> dispersion in the spectral accelerations for Bin 1b is negligible.<br />

<strong>The</strong> 16th, 50th and 84th percentiles and β of the inelastic peak displacement for Bin 1b are shown in Figure<br />

22 together with those for Bin 1a. <strong>The</strong> results indicate that the use of spectrally matched ground motions<br />

underestimate the median peak displacement demand in highly nonlinear SDOF systems and cannot capture the<br />

dispersion in the displacement response. For Fy<br />

= 0.06W<br />

(see Figure 22e), the median responses are<br />

underestimated by 20%. This observation is similar to that of Bazzurro and Luco (2006) for NF motions.<br />

Earthquake ground motions that are spectrally matched to a target median spectrum should not be used for risk<br />

computations of nonlinear SDOF systems and first-mode-dominated structures because a) the median<br />

displacement response will be underestimated, and b) the dispersion in the displacement response is<br />

underestimated by a wide margin.<br />

y<br />

-386-

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