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8.3 ERA<br />

ERA results during monitoring are summarized in Table 8.1. ERA on a PC using the<br />

same data gives the same results numerically. Note that the structure has undergone some<br />

structural changes since the data injected to Imote2 networks in Chapter 7 was acquired;<br />

some of connections were tightened and some of elements were adjusted. The identified<br />

natural frequencies in Table 8.1 are not necessarily same as those in Table 7.3. By<br />

comparing the identified natural frequencies with the cross-spectral density plots in Figure<br />

8.6, the identified natural frequencies are considered to well capture the dynamic<br />

characteristics of the signals.<br />

Table 8.1. Identification of Natural Frequencies and Damping Ratios<br />

Natural Frequency (Hz) Damping Ratio (%)<br />

20.7229 2.9321<br />

32.8985 0.2127<br />

41.2990 0.4846<br />

64.3174 0.2422<br />

69.1086 0.3718<br />

94.9259 0.2810<br />

8.4 DLV methods<br />

The DLV method based on the mass perturbation and SDLV methods are applied to<br />

the modal parameters identified before and after damage. The mass perturbation DLV<br />

method, involving initialization to determine the mass normalization constants is first<br />

examined. Subsequently, the SDLV method is investigated.<br />

The mass normalization constants to be used in the mass perturbation DLV method<br />

are first estimated. Imote2s are installed at nodes 7, 9, 11, 13, 15, 17, 19, 21, 23, and 25.<br />

Measurements are taken before and after additional mass is attached to node 11. The mass<br />

is 1.253 kg. All the nodes measure vertical acceleration. The node at the location of the<br />

additional mass measures acceleration in the longitudinal and transverse directions as<br />

well, because the denominator of Eq. (6.21) requires mode shapes at the degrees-offreedom<br />

corresponding to the mass perturbation, i.e., acceleration in all three directions is<br />

needed. Thus, acceleration is measured in 12 channels. The mass normalization constants<br />

are estimated and listed in Table 8.2, as well as natural frequencies of the structure with<br />

and without the mass perturbation.<br />

The identified mass normalization constants are utilized to reconstruct the flexibility<br />

matrix as shown in Eqs. (6.19) and (6.32). Imote2s monitoring sensor communities 1, 2,<br />

and 3 reconstruct the flexibility matrices before and after element 8 is replaced with an<br />

element of reduced cross-section. The Imote2s then perform an SVD on the difference in<br />

the flexibility matrices to estimate the DLVs. The DLVs are then multiplied by a matrix to<br />

convert nodal force to element stresses. Elements with small stresses are identified as<br />

141

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