Chiou and Youngs PEER-NGA Empirical Ground Motion Model for ...
Chiou and Youngs PEER-NGA Empirical Ground Motion Model for ... Chiou and Youngs PEER-NGA Empirical Ground Motion Model for ...
with increasing rupture depth. The data in the PEER-NGA data set are insufficient to test if Equation (13) performs better than piece-wise linear functions of RRUP, M and ZTOR. SITE EFFECTS Near-Surface Geology: The incorporation of the effects of near-surface geology or site classification has gone through an evolution in the past 10 years. At the beginning of this period, ground motion models typically contained a scaling parameter based on site classification (e.g. Boore et al., 1993), or presented different models for “rock” and “soil” sites (e.g. Campbell, 1993; Sadigh et al. 1997). Classification of recording sites into rock or soil sites varied among investigators. Boore et al. (1997) introduced the explicit use of the average shear wave velocity in the upper 30 meters, VS30, in the ground motion model. Abrahamson and Silva (1997) building on an earlier model by Youngs (1993) introduced the explicit modeling of non-linear site effects in the ground motion model. The model we have developed for incorporating near-surface geology combines these concepts. ln( site ref Site S 30 ref y ) = ln( y ) + f ( V , y ) (14) The parameter yref is the ground motion on the reference site condition derived from the source and path scaling models described in the previous section. The reference site shear wave velocity was chosen to be 1130 m/sec because of the initial use of site response data to develop the functional form (Silva, 2004) and because it is expected that there will not be significant nonlinear site response at this velocity. As indicated on Figures 4 and 5, there are very few data with values of VS30 greater than 1100 m/sec. The reference motion is defined to be the spectral acceleration at the spectral period of interest for two reasons. Bazzurro and Cornell (2004) indicate that the spectral acceleration at spectral period T is “the single most helpful parameter” for the prediction of site amplification at that period. In addition, the estimation of the coefficients of the ground motion model is performed using random (mixed) effects regression in which the reference motion includes the random event term representing the deviation of the average ground motions from a given earthquake from the global population mean. Use of the reference spectral acceleration at period T to estimate surface ground motions at the same period eliminates the need to include the correlation in the random effects between those at period T and those at another period, such as pga at “zero” period. The function form for the site response model fSite with yref = SA1130 is given by: where f Site ( V S 30 , T, SA 1130 ) = a( V a( V S 30 S 30 , T ) + b( V b( Vs30, T ) = φ ( T ) exp 2 ⎡ VS 30 ⎤ , T ) = φ1 ln⎢1130⎥ ⎣ ⎦ c( T ) = φ ( T ) ⎡ SA1130 ( T ) + c( T ) ⎤ , T ) ln⎢ c( T ) ⎥ ⎣ ⎦ { φ ( T ) × ( V − 360) } C&Y2006 Page 29 4 3 S 30 S 30 (15)
The interpretation of the parameters a, b, and c is illustrated in Figure 23. Parameter a represents the linear site response that occurs at small level of reference site motion. It is modeled as a linear function of ln[VS30] consistent with previous representations (e.g. Boore et al., 1997). Parameter c represents the ground motion level in the middle of the transition from linear to nonlinear behavior. Parameter b represents the nonlinear behavior in terms of a linear decrease in the natural log of site amplification, fS, with increasing amplitude of the reference motion. In general, a stronger nonlinearity in soil response corresponds to a more negative value for b (stronger dependence on SA1130). It is expected that the degree of nonlinearity is a function of the stiffness of the site soils and is represented by making b a function of VS30. fSite a c Figure 23: Soil amplification function ln(SA1130) The ability of Equation (15) to represent nonlinear site response is illustrated in Figures 24 and 25. Figure 24 shows site amplification factors for pga derived from Silva’s (2004) simulations. Two soil property models were used by Silva (2004), the EPRI (1993) set of soil modulus and damping relationships and the less nonlinear set Peninsular Range set developed by Silva et al. (1996). The solid lines shown on the figure are the result of fitting Equation (15) to the combined amplification factors for the two soil model sets and indicate that the function form can well represent the behavior implied by nonlinear (equivalentlinear) site response. Figure 25 shows the values of parameters a and b derived from the results of Silva (2004). The dashed lines show that the function forms for a and b in Equation (15) provide a good match to the site response results. C&Y2006 Page 30 b
- Page 1 and 2: Chiou and Youngs PEER-NGA Empirical
- Page 3 and 4: data are consistent with strong mot
- Page 5 and 6: Figure 1: Magnitude-distance-region
- Page 7 and 8: Figure 2: Empirical ground motion d
- Page 9 and 10: EQID Earthquake M Table 3: Inferred
- Page 11 and 12: Site Average Shear Wave Velocity: A
- Page 13 and 14: Figure 6: Relationship between VS30
- Page 15 and 16: 1 ) ∝ C2 × M + ( C2 − C ) × l
- Page 17 and 18: Figure 9: Peak acceleration data fr
- Page 19 and 20: C4+C5M slowly and the value of the
- Page 21 and 22: allows the interpretation of the co
- Page 23 and 24: Figure 13: Coefficients resulting f
- Page 25 and 26: the top of rupture located at x = 0
- Page 27 and 28: Figure 18: Intra-event residuals fo
- Page 29: Figure 21: Variation of HW* with ma
- Page 33 and 34: to the PEER-NGA pga data selected f
- Page 35 and 36: EFFECT OF DATA TRUNCATION The initi
- Page 37 and 38: term [ 1 Φ( y ( θ ) + τ ⋅ z ,
- Page 39 and 40: Table 4: Estimate of Anelastic Atte
- Page 41 and 42: data truncated at a maximum distanc
- Page 43 and 44: faulting earthquakes at long period
- Page 45 and 46: Slope -1.5 -1.0 -0.5 0.0 0.5 1.0 0.
- Page 47 and 48: C&Y2006 Page 46 Table 5: Coefficien
- Page 49 and 50: c1 of T0.010S c1 of T1.000S MODEL R
- Page 51 and 52: esid 1 0 -1 -2 resid resid 1 0 -1 -
- Page 53 and 54: esid resid resid 1 0 -1 -2 1 0 -1 -
- Page 55 and 56: esid 2 1 0 -1 -2 SCEC Version 2 0 2
- Page 57 and 58: Amplification w.r.t. Vs30 = 1130 m/
- Page 59 and 60: Sa(g) Sa(g) 10 1 0.1 0.01 10 1 0.1
- Page 61 and 62: Sa (g) Sa (g) 1 0.1 0.01 0.001 0.00
- Page 63 and 64: Sa (g) Sa (g) 1 0.1 0.01 0.001 1 0.
- Page 65 and 66: EXAMPLE CALCULATIONS FORTRAN routin
- Page 67 and 68: Table 6: Example Calculations Perio
- Page 69 and 70: REFERENCES Abrahamson, N.A., and Si
- Page 71 and 72: Frankel, A., A. McGarr, J. Bicknell
- Page 73 and 74: Appendix A Recordings from PEER-NGA
- Page 75 and 76: RSN EQID Earthquake M Station No, S
- Page 77 and 78: RSN EQID Earthquake M Station No, S
- Page 79 and 80: RSN EQID Earthquake M Station No, S
The interpretation of the parameters a, b, <strong>and</strong> c is illustrated in Figure 23. Parameter a<br />
represents the linear site response that occurs at small level of reference site motion. It is<br />
modeled as a linear function of ln[VS30] consistent with previous representations (e.g. Boore<br />
et al., 1997). Parameter c represents the ground motion level in the middle of the transition<br />
from linear to nonlinear behavior. Parameter b represents the nonlinear behavior in terms of<br />
a linear decrease in the natural log of site amplification, fS, with increasing amplitude of the<br />
reference motion. In general, a stronger nonlinearity in soil response corresponds to a more<br />
negative value <strong>for</strong> b (stronger dependence on SA1130). It is expected that the degree of<br />
nonlinearity is a function of the stiffness of the site soils <strong>and</strong> is represented by making b a<br />
function of VS30.<br />
fSite<br />
a<br />
c<br />
Figure 23: Soil amplification function<br />
ln(SA1130)<br />
The ability of Equation (15) to represent nonlinear site response is illustrated in Figures 24<br />
<strong>and</strong> 25. Figure 24 shows site amplification factors <strong>for</strong> pga derived from Silva’s (2004)<br />
simulations. Two soil property models were used by Silva (2004), the EPRI (1993) set of<br />
soil modulus <strong>and</strong> damping relationships <strong>and</strong> the less nonlinear set Peninsular Range set<br />
developed by Silva et al. (1996). The solid lines shown on the figure are the result of fitting<br />
Equation (15) to the combined amplification factors <strong>for</strong> the two soil model sets <strong>and</strong> indicate<br />
that the function <strong>for</strong>m can well represent the behavior implied by nonlinear (equivalentlinear)<br />
site response. Figure 25 shows the values of parameters a <strong>and</strong> b derived from the<br />
results of Silva (2004). The dashed lines show that the function <strong>for</strong>ms <strong>for</strong> a <strong>and</strong> b in<br />
Equation (15) provide a good match to the site response results.<br />
C&Y2006 Page 30<br />
b