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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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ACOUSTIC LENSES<br />

- 107 -<br />

Ten acoustic lenses were designed to cover the range of wall thicknesses<br />

and weld preparations suggested for inspection. Selection of defects for<br />

inclusion in the program finalized the inspection requirements (inspection<br />

angle, defect location), and four lens/wedge/transducer combinations were<br />

then chosen to be used. Each assembly was calibrated by signal amplitude<br />

and time—of-flight using a calibration block containing 1.5 ram diameter<br />

side drilled holes spaced 2.5 and 4.0 mm apart (Figure 2a). The high<br />

resolution capability of focused beams is readily capable of<br />

differentiating between such small targets (Figure 2c) in contrast to the<br />

broad beam results for a standard transducer (Figure 2b). The calibration<br />

data was used to determine the beam inspection angle and time-of-flight of<br />

sound in the lens/wedge assembly.<br />

DEFECT SIZING<br />

Each weld specimen was examined ultrasonically from both sides of the outer<br />

surface weld bead using a simple scanning mechanism (Figure 1). The<br />

pulse-echo technique, which is commonly used in the field, was used<br />

throughout in contact mode with a light oil as couplant. The inspection<br />

data was recorded as multiple A-scans. In this technique, the probe is<br />

incrementally moved axlally away from the weld bead. The gate of the<br />

ultrasonic instrument is swept across the CRT screen, and the signal<br />

amplitude versus time display (shown on the CRT) is plotted for each probe<br />

position (see Figure 3). As the path length to the defect increases, the<br />

time-of-flight increases and the defect response on the A-scan moves to the<br />

right on the time axis. Conversely, any extraneous signal (e.g. from the<br />

lens/wedge assembly) remains at constant time and is readily<br />

distinguishable on the multiple A-scan record. The through-wall depth of<br />

the defect can then be calculated based on the extent of the defect<br />

response along the time axis.<br />

Metallurgical Examination<br />

After ultrasonic examination, each specimen was broken open by cooling it<br />

in liquid nitrogen and using three point impact loading to fracture along<br />

the centre of the weld. Where samples did not break through the defect<br />

(primarily for the smaller buried defects) the sample was sectioned and<br />

metallographically prepared to reveal the defect size.<br />

RESULTS<br />

A typical inspection record (Figure 4a) and specimen cross-section (Figure<br />

4b) are shown for a planar root crack giving a comparison of predicted<br />

versus actual defect size. These results are representative, as in all<br />

cases size predictions were in good agreement with the actual defect<br />

depths. This excellent correlation is further illustrated in Figure 5<br />

where the majority of data points fall within a band +1.5 mm of the line as<br />

determined by regression analysis. The 95% confidence limits for the<br />

predicted mean flaw depths are shown. There was little distinction in<br />

sizing accuracy between volumetric and planar defects. The technique is<br />

conservative in that defects tend to be slightly oversized (average error<br />

was 0.37 mm).

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