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539<br />

in which<br />

H = [H(t l ), H(t 2 ), -.., H(t L )] T (2.3)<br />

0 = [c 13 c 2 , -.., C N , k p k 2 , .... k N f (2.4)<br />

P = [P(t l ), P(t 2 ), »., P(t L )f (2.5)<br />

where H is the response matrix of velocity and displacement of the building. H is a rectangular<br />

matrix of order (L x N) x J, where L is the number of sampling points in the measured structural<br />

response time history and J is the number of unknown parameters. For the present case, J =2*N.<br />

Vector 9 contains all the unknown parameters and P is a vector related to the ground acceleration<br />

and building inertia forces.<br />

At any sample time instant t,, one has<br />

H(t,) =<br />

"*,<br />

0<br />

X 1 -x 2 0<br />

x 2 — x, x, — x 3<br />

0<br />

0<br />

x, x,-x, 0 0<br />

0 x,-x t x 2 -x 3 0<br />

(2.6)<br />

0<br />

0 0<br />

x n -x<br />

0 0 0 x n »x Q<br />

P(t 1 ) = [-m l x 1 (t l )-m l x g (t t ), -m.jXjtt.J-mjX^t,), •••, -m N x N (t l )-m N x g (t l )] r (2J)<br />

<strong>The</strong> responses of the structure are supposed to be measured in terms of displacement, velocity and<br />

acceleration. If the ground acceleration X g (t) is available, parameter estimation is trivial using, for<br />

instance, the least-squares technique (Hsia, 1977) as<br />

0 = [H T H] 1 H T P (2>8)<br />

However, the problem here is the ground acceleration is unknown and it is expected to simultaneously<br />

estimate with the structural parameters. In this connection, a dynamic compound inverse method is<br />

suggested below.<br />

Dynamic Compound Inverse Method<br />

<strong>The</strong> dynamic compound inverse method is actually an iterative identification procedure that consists of<br />

the least-squares technique for parameter identification and the statistical average method for forcing<br />

the identified input excitation to comply with the dynamic equilibrium of the concerned building. <strong>The</strong><br />

implementation of the dynamic compound inverse method can be divided into the following steps.<br />

Stepl: Since both the structural parameters 0 and the ground motion X g (t) are unknown, initial<br />

values for the structural parameters have to be assumed, for instance, let 9 Q = [l, 1, •••, l] T . It will<br />

be demonstrated later that the performance of the suggested method is not sensitive to this initial<br />

assumption. <strong>The</strong> symbol ' A ' stands for the estimated value and the subscript 4 0* of 0 stands for the<br />

number of iteration times.<br />

Step2i From Eqn.2.2, the vector P can be estimated using # 0 and the measured structural responses,<br />

resulting in P = H0 0 . <strong>The</strong>n, comparing with Eqn.2.7, one may have

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