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4 - Memorial University of Newfoundland DAI

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n new valuc<strong>of</strong> FPB(M) or AIC[M) excecda the previous one; the iteration<br />

is then lerminatod. (Both eritcria are "red in this trealiro.)<br />

6.3 Estimating Modal Parameters<br />

R~timnting rcnonnnt frcqoency and damping ratio. from the MEM spectral<br />

vs~imntc (i.. . oquation (6.22) does no1 immediatelyappear to have any great<br />

advnntngc over convrntional methods (PFT). But when the expression is re-<br />

oxamincd, it i. ohscrved that the ~peclml estimate is axtually a closed-form<br />

egtrnatian lor the re3pon.c rprrtrum. This ~ni~ucfestureol the MEM spectral<br />

cstim;sc provides the key to formulating the nlodal pnran~eterertimators and<br />

their s1ntistics.<br />

6.3.1 Resonant Frequencies<br />

Itesonnd fqucncics can be estimated as the selection <strong>of</strong> frequencies corn<br />

sponding to relative maximum <strong>of</strong> the corresponding spectrum. This search<br />

for t~~aximnem be expressed in s mathematical form using the result <strong>of</strong> dif-<br />

fcrotltinl calculations which slates: the derivative <strong>of</strong> s function is zero at an<br />

extrema. Thus, as the spectrum is avnilable in the functional form, the rela-<br />

livc cvtrenla <strong>of</strong> the spectral density spectrum can be abtsined rn the solution<br />

or:<br />

-- dC*.<br />

df - O.<br />

(6.29)<br />

To obtain an expression which satisfiesequation (6.29), the following steps<br />

are lskcn:<br />

Let

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