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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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- 334 -<br />

It is also possible to do the reverse and transform the complex frequency spectra into time spectra;<br />

Figure 8 is an example o[ this for a 90 pm void. Transformations for void sizes from 28 urn to 132 urn<br />

diameter show that the fargest deflection from zero was negative-going. In Figures 9a-d, peak<br />

deflections versus time have been plotted with the largest negative-going deflection normalized to -<br />

100%. From this figure, it is evident that as the void diameter increases, the largest positive-going<br />

deflection changes from the one following the largest negative-going deflection to the positive-going<br />

deflection preceding it. This behaviour has been noted previously in the experimental results.<br />

Plotting ratios of these two positive going peaks against the void dimensions (fig. 10) shows that there<br />

exists a reasonable correlation with the minor dimension of the void. Although a similar relation<br />

exists with the major void dimensions it is less apparent, especially for the larger dimensions which<br />

approach or exceed the wavelength, \c, of the main frequency component..<br />

V. C<strong>ON</strong>CLUSI<strong>ON</strong>S<br />

Calculations have shown that trends apparent in-signals reflected from voids in the focal zone of<br />

pulsed focused transducer can be reproduced by a model based on scattering of monochromatic plane<br />

waves convoluted with the frequency distribution of the incoming wavepacket. Although direct<br />

signal amplitude comparison of theory and experiment is not possible due to lack of information about<br />

the focal zone pressure, comparison of normalized signals show strong correspondences in signal<br />

shape. The calculated changes of the frequency distribution as a function of void diameter as<br />

measured by the frequency at maximum amplitude and frequency full width at half maximum have<br />

been followed closely by the measured values.<br />

The ratio of the positive going signal peaks in the time spectra have proven to be related to the size of<br />

the reflector and the wavelengths used. It can be used as a practical tool for absolute sizing without<br />

the use of artificial reference.<br />

REFERENCES<br />

1. Proceedings of the DARPA/AFWAL Review of Progress in Quantitative NDE (1981).<br />

2. Van den Andel, J Stockman, A., and Nicholson, P.S., "The Importance of Correct Alignment<br />

in Ultrasonic Testing", Advanced NDE Technology, Bussiere, J.F. ed., NRC Canada, 1982, p.<br />

21.<br />

3. Nicholson, Stockman and Van den Andel, "Ultrasonic Detection of Defects in High<br />

Performance Ceramics", CSNDT Journal, Vol. 4, No. 2, Nov. 1982.<br />

4. Ying, CF. and Truell, R., "Scattering of a Plane Longitudinal Wave by a Spherical Obstacle<br />

in an Isotropically Elastic Solid", J. Appl Phys.36, 1086(1956).<br />

5 Tittmann, B.R., Cohen, R.E. and Richardson. J.M., "Scattering of Longitudinal Waves<br />

Incident on a Spherical Cavity in a Solid", J. Acoust. Soc. Am, 63, 68(1978).

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