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[23, 37]. A higher voltage helps to generate stronger Lamb waves with a larger signal to noise<br />

ratio but at the cost of high power consumption [38]. High power consumption is not<br />

recommended as SHM systems typically have requirements of low power. A voltage of 5-10<br />

V has <strong>be</strong>en found to <strong>be</strong> optimum for most SHM applications. A signal with a larger num<strong>be</strong>r<br />

of peaks has a higher energy associated with it. This aspect helps in long distance propagation<br />

as it compensates for any attenuation due to damping. However, increasing the num<strong>be</strong>r of<br />

peaks increases the pulse width and, in turn, the interference [39, 40]. A three to five cycle<br />

Hanning modulated tone burst has <strong>be</strong>en shown to <strong>be</strong> an optimal form of actuation <strong>be</strong>cause<br />

this method allows separating the anti-symmetric and symmetric modes and allows<br />

separating the reflection from the edges or from cracks [41]. Diamanti and Soutis [42] studied<br />

the use of low frequency for composite damage detection. Lower frequencies excite a smaller<br />

num<strong>be</strong>r of modes making them more distinguishable. The first order anti-symmetric (A0)<br />

mode has a smaller wavelength for a given frequency compared to the first order symmetric<br />

(S0) mode making A0 waves more sensitive to small levels of damage. In addition, S0 modes<br />

undergo higher attenuation during propagation [24, 40]. Given these characteristics, a five<br />

cycle tone burst of 1 kHz center frequency and an amplitude of 6 V to generate A0 mode<br />

Lamb waves was considered in the testing protocol. The excitation input signal is shown in<br />

Figure 2.2.<br />

Figure 2.2. A typical PZT excitation input signal for the testing scheme used in this study.<br />

11

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