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The eigenproblem of the system matrix is then solved:<br />

D – 1/2 P T H rs kQD – 1/2 i = z i i<br />

(6.11)<br />

The natural frequencies f i<br />

and damping ratios i<br />

are then calculated from the eigenvalues,<br />

z i<br />

as<br />

i z i kt<br />

=<br />

<br />

<br />

f i<br />

= i<br />

<br />

i<br />

=<br />

Re( i<br />

) i<br />

<br />

(6.12)<br />

where z i<br />

is the principal value of natural logarithm of z i<br />

. t is the sampling period.<br />

Re takes the real part of a complex number. The mode shape, i<br />

, corresponding to z i<br />

is calculated as<br />

i<br />

= PD 1/2 i<br />

. (6.13)<br />

E p<br />

T<br />

The initial modal amplitudes, , which can be utilized to calculate modal amplitude<br />

coherence, an indicator to quantitatively distinguish the system and noise modes, is<br />

estimated as follows:<br />

<br />

=<br />

-1 D 1/2 Q T E m<br />

(6.14)<br />

6.3 Damage Locating Vector method<br />

One of the flexibility-based SHM approaches is the Damage Locating Vector (DLV)<br />

method, which is briefly described here. The DLV method, first developed by Bernal<br />

(2002), is based on the determination of a special set of vectors, the so-called damage<br />

locating vectors (DLVs). These DLVs have the property that when they are applied to the<br />

structure as static forces at the sensor locations, no stress is induced in the damaged<br />

elements. This unique characteristic can be employed to localize structural damage (Gao,<br />

2005).<br />

For a linear structure, the flexibility matrix, F , at the sensor locations is constructed<br />

from measured data. Gao (2005) explained two approaches to estimate the flexibility<br />

matrix. Both of them reconstruct the flexibility matrix using mode shapes and<br />

normalization constants. One approach estimates the normalization constants assuming<br />

that the input force can be measured, while the other utilizes output-only measurements<br />

before and after a known mass perturbation.<br />

Formulation of the flexibility matrix based on input force measurements is<br />

summarized by the following equation involving complex conjugate pairs of arbitrary<br />

normalized mode shapes, = .<br />

94

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