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Proceedings e report - Firenze University Press

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STRUCTURAL DEFECT DETECTION USING ACOUSTIC HOLOGRAPHY – A PRELIMINARY STUDY<br />

• except for the excitation process, it is a non contact method<br />

• since an important number of grid points (120) can be measured at the same time, the number of<br />

excitation impacts on the structure is strongly limited.<br />

• The measurement time is comparatively very short.<br />

In the present study it took less than 120 mn for recording the set of 15360 point impulse responses to<br />

be processed.<br />

3.2. Experimental set-up<br />

The impulse response of the harpsichord soundboard is measured in the semi-anechoic chamber at the<br />

Musée de la Musique (Fig. 4 (a)). This experiment is described in [5]. In such a room noise level is<br />

seriously attenuated. This condition allows minimizing the soundboard excitation level and also<br />

optimizing the signal to noise ratio for evanescent waves.<br />

Since the instrument has to be kept under tension, the strings are muffled in order to eliminate their<br />

sound production (Fig. 4(b)).<br />

(a) (b) (c)<br />

Fig. 3 NAH experimental set up: (a) holographic microphone array, (b) string muffling (c) impact hammer<br />

The impulse response is calculated from the measured harmonic acoustic nearfield using a NAH<br />

reconstruction process. A point impulse excitation of the soundboard is provided by an automated<br />

hammer driven by an electromagnet that produces a reproducible impact (Fig. 4(c)). The excitation<br />

position is chosen on the underside of the soundboard. The keyboard is therefore removed. The<br />

position of the impact is chosen so as to mobilize significant flexural vibration modes of the<br />

soundboard.<br />

A 12 by 10 electret microphones array, with a 50 mm step, has been used to collect the pressure field.<br />

So as to fit the measurement grid, the array is moved into 8 positions. For each of these positions the<br />

array is also moved according to 16 interleaved positions so as to refine the measurement step grid to<br />

12.5 mm. The 120 impulse pressure responses for each position of the array are collected using a<br />

home-made 128 channels synchronous digital recorder. Each measurement associated to one impact<br />

on the soundboard has to be phase referenced by systematically recording, along with the acoustic<br />

signals, the constant impulse response of an accelerometer positioned on the soundboard. The<br />

resulting acoustic impulse response field is measured over a parallel plane at a distance zh = 72 mm.<br />

This unusually large distance for NAH has been imposed by technical reasons of accessibility. The<br />

field is finally sampled according to a 1162.5 by 1762.5 mm rectangle grid with a 12.5 mm step. The<br />

different sets of measurement finally count 13348 point acoustic impulse responses (Fig. 4).<br />

3.3. Radiated sound pressure<br />

On Fig. 5, we present the pressure level, averaged on the whole measurement plane, from 0 to<br />

2000Hz. This graph shows a significant radiation level for frequencies between 140 Hz and 2000 Hz.<br />

An important modal density in the usable [0 2000Hz] bandwidth can be observed.<br />

The frequency response depends on the geometry, the material, the limits condition, and on the<br />

environmental conditions during the experiments. This frequency spectrum is the response of the<br />

structure for a mechanical state: it is a sort of the identity signal of the harpsichord.<br />

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