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measurement or mass perturbation can be greatly simplified with the SDLV method. The<br />

SDLV method is briefly reviewed in this section.<br />

Bernal (2006) stated that the null space of the change in the flexibility matrix will be<br />

contained in the null of Q T . The matrix Q T is the transpose of the change in Q which<br />

is defined as follows:<br />

Q = – CA – p<br />

+ <br />

H † p L<br />

(6.33)<br />

H<br />

CA – p<br />

p<br />

=<br />

CA – p<br />

(6.34)<br />

L<br />

=<br />

I<br />

<br />

(6.35)<br />

where I denotes identity matrix, denotes a zero matrix. p = 0, 1, or 2, depending on<br />

whether the measured outputs are displacement, velocity, or acceleration. The system<br />

matrix A and observation matrix C are determined through modal analysis such as ERA.<br />

The null vectors of Q T are treated as DLVs.<br />

Bernal (2006) also proposed a way to determine the number of DLVs and to combine<br />

information from multiple DLVs. When there are q DLVs and the stress corresponding to<br />

each vector is j<br />

, a normalized stress index (nsi) is defined as follows:<br />

j<br />

nsi j<br />

=<br />

--------------<br />

j max<br />

(6.36)<br />

Weighting can be incorporated to yield a weighted stress index (WSI) as<br />

WSI =<br />

q<br />

<br />

j=1<br />

j<br />

nsi j<br />

(6.37)<br />

where is a weighting parameter. Potentially damaged elements ( PD ) are chosen as<br />

j<br />

PD = elements|WSI<br />

tol<br />

(6.38)<br />

Bernal (2006) took j = and tol = 0.1 WSI max<br />

. The number of DLVs, q , can be<br />

estimated as<br />

<br />

q = # of values <br />

<br />

<br />

=<br />

s i<br />

<br />

------------ <br />

<br />

s j max<br />

(6.39)<br />

100

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