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Chiou and Youngs PEER-NGA Empirical Ground Motion Model for ...

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MODEL PARAMETER DEVELOPMENT<br />

The general <strong>for</strong>m of the ground motion model used to assess the model parameters is shown<br />

in Equation (16):<br />

f<br />

Source<br />

f<br />

= c (<br />

Path<br />

f<br />

HW<br />

2<br />

4<br />

9<br />

[ y ]<br />

[ 1+<br />

exp{<br />

c ( c − M ) } ]<br />

3<br />

M n M<br />

= c ln<br />

b<br />

2 2<br />

[ RRUP<br />

+ c5<br />

cosh{<br />

c6<br />

max( M − cHM<br />

, 0 ) } ] + ( c4a<br />

− c4<br />

) × ln[<br />

RRUP<br />

+ cRB<br />

]<br />

= φ ×<br />

[ c + c / cosh{<br />

max( M − c , 0}<br />

]<br />

tan<br />

/ 2 ) ×<br />

⎧ ⎡ VS<br />

30 ⎤ ⎫<br />

= φ1<br />

min⎨ln<br />

⎢<br />

0⎬<br />

+<br />

⎩ ⎣1130⎥<br />

, b<br />

⎦ ⎭<br />

2<br />

γ 1<br />

1130<br />

⎛ c2<br />

− c ⎞<br />

− 6 ) + ⎜<br />

⎟ × ln<br />

⎝ cn<br />

⎠<br />

f<br />

⎧ W cos( δ ) ⎫<br />

⎨ ⎬<br />

⎩2(<br />

ZTOR<br />

+ 1)<br />

⎭ ⎧<br />

× ⎨1−<br />

π / 2 ⎩ R<br />

{ ln[ y ] }<br />

[ exp{<br />

φ ( min( V , 1130 ) − 360)<br />

} − expφ<br />

( 1130 − 360)<br />

]<br />

3<br />

] = c<br />

γ 2<br />

2<br />

= c cos ( δ ) × tanh( R<br />

Site<br />

Site<br />

ln<br />

ln[ y<br />

Surface<br />

RUP<br />

= ln[ y<br />

1<br />

+<br />

f<br />

S 30<br />

1130<br />

Source<br />

] + f<br />

−1<br />

R ⎫<br />

JB<br />

⎬<br />

+ 0.<br />

001⎭<br />

− 4 )<br />

C&Y2006 Page 33<br />

+<br />

Site<br />

f<br />

Path<br />

Site<br />

+<br />

γ 3<br />

+ σ ⋅ z<br />

f<br />

HW<br />

+ c<br />

+ τ ⋅ z<br />

1a<br />

× R<br />

ij<br />

F<br />

RUP<br />

3<br />

RV<br />

+ c<br />

1b<br />

F<br />

NM<br />

RUP<br />

⎡ exp 1130 + φ ⎤ 4<br />

ln⎢<br />

⎥<br />

⎣ φ4<br />

⎦<br />

i<br />

+ c ( Z<br />

The parameter y1130 is the ground motion on the reference site condition (VS30 = 1130 m/sec).<br />

Its level is based on the source scaling function fSource, the path scaling function, fPath, the<br />

hanging wall function fHW, <strong>and</strong> a r<strong>and</strong>om effect τ zi that is modeled as a Gaussian r<strong>and</strong>om<br />

variate with inter-event st<strong>and</strong>ard deviation τ. The log of the ground motion at a site is the<br />

sum of the log of the reference motion <strong>and</strong> a nonlinear amplification, fSite, that is a function of<br />

VS30 <strong>and</strong> the level of the reference motion. The ground motions at the site also include a<br />

r<strong>and</strong>om Gaussian variate with intra-event st<strong>and</strong>ard deviation σ. The inter-event component<br />

of r<strong>and</strong>omness in included when computing the site amplification. Also note that the site<br />

amplification function uses the reference motion <strong>for</strong> the same spectral period. The additional<br />

parameters in Equation (16) are: RRUP , closest distance to the rupture plane (km); RJB ,<br />

Joyner-Boore distance to the rupture plane (km); δ , rupture dip; W , rupture width (km); ZTOR<br />

, depth to top of rupture (km); FRV , reverse faulting factor equal to 1 <strong>for</strong> 30º ≤ λ ≤ 150º, <strong>and</strong> 0<br />

otherwise; FNM , normal faulting factor equal to 1 <strong>for</strong> -120º ≤ λ ≤ -60º, 0 otherwise; λ , slip<br />

rake angle; VS30 , average shear wave velocity <strong>for</strong> top 30 m (m/s). Note, fHW applies to all<br />

faulting styles.<br />

The model parameters were obtained by fitting the model to the selected <strong>PEER</strong>-<strong>NGA</strong> data<br />

using the nonlinear mixed effects method nlme implemented in the statistical packages S-<br />

Plus <strong>and</strong> R. The process used to obtain these parameters is described below.<br />

7<br />

TOR<br />

+<br />

(16)

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