Civil Engineering Reference
In-Depth Information
×
m identify matrix, this is because the means U i and U j is uncorrelated, for
i
j .
Substituting Eq. [12.22] into Eq. [12.20] and Eq. [12.21], the mean vector
and covariance matrix of Z can be reduced to
t
t
[12.23]
MA0BB d
=+=
S
=
AIAAA
=
Z
ZZ
Because Y and Z are both joint normal distribution, if the mean vector
and covariance matrix of Z matches the mean vector and covariance matrix
of Y , Y and Z will have the same joint normal distribution. Equations
[12.24] and [12.25] show the selection of A and B such that Z will have the
same joint normal distribution as Y .
MM BM
Z
=⇒=
[12.24]
Y
Y
[
(
)
]
t
t
[12.25]
SS S S
ZZ
=
⇒ =
AA
⇒=
A
chol
YY
YY
YY
where chol is the Choleski factorization of any square and positive defi nite
matrix.
Because the entry of the covariance matrix is not bounded, the computa-
tion might cause numerical instability. The Choleski factorization of
Σ
YY is
calculated using Eq. [12.26].
S
=
DR D
AA
t
=
DR D
A
[12.26]
YY
YYYY
YYYY
[
(
)
]
t
[
(
)
]
t
=
chol
DR D
=
D
chol
R
=
DD YY
YYYY
Y
YY
where D Y is a diagonal matrix with standard deviations of random variables
Y along its diagonal and R YY is the correlation coeffi cient matrix of random
variables Y . By substituting Eqs. [12.24] and [12.26] into Eq. [12.19], the
correlated EDP vector can be generated using Eq. [12.27].
ZDLUM
YY
=
+
[12.27]
Y
Finally, the generated EDP vectors are transformed to the lognormal
distribution, W , by taking the exponential of Z . Figure 12.6 summarizes the
process of generating correlated EDP vectors.
12.3
Application: seismic performance assessment of
high-rise buildings
This section shows an example of applying the performance-based assess-
ment procedure to compare the seismic performance of a high-rise building
designed using three design approaches. Effectiveness of the design methods
is assessed using the repair costs associated with anticipated earthquake
ground shaking.
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