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Engine Titanium Consortium - Center for Nondestructive Evaluation ...

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the high-noise coupons shown in the figure, resulting in 30.6%, 43.0% and 36% <strong>for</strong> the PW, HW<br />

and GE coupons respectively.<br />

In addition to the S/N measurements, sonic pulse volumes were also measured. First, the –6dB<br />

beam diameter at the FBH depth was determined from a fine increment C-scan of the reference<br />

hole in the PW coupon. Figure 4 illustrates the beam diameter determination <strong>for</strong> the same<br />

example, leading to a value of 39.4 mils. Secondly, as illustrated in Figure 5, the pulse duration<br />

was measured by finding the –6 dB points <strong>for</strong> the envelope function of the rectified FBH echo, and<br />

this duration was translated to a pulse length in metal. For the case shown, the pulse length was<br />

36.7 mils, leading to a measured pulse volume of (π/4)(39.4 mils) 2 (36.7mils) = 44,600 cubic mils.<br />

Peak noise vs. pulse volume <strong>for</strong> all measurements is summarized in Figure 6.<br />

PW8<br />

Max. noise<br />

30.6%<br />

HW5<br />

Max noise<br />

43%<br />

GE6<br />

Max. noise<br />

36%<br />

#1/2 FBH ~ 80%<br />

Figure 3. Example of S/N measurements in high-noise <strong>for</strong>ging coupons. Here the FBH holes are<br />

located at the focus of an F6 transducer.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 61

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