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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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- 251 -<br />

absorption, the conversion of acoustic energy into heat. Scattering and<br />

absorption are both caused by the presence of inhoraogeneities such as<br />

precipitates, inclusions, voids, grain and interphase boundaries,<br />

dislocations, interstitial impurities, etc. Since these same inhomogeneities<br />

also play a primary role in determining mechanical properties, it is expected<br />

that measurements of attenuation will reflect mechanical properties. The<br />

sensitivity of attenuation to small changes in microstructure which affect<br />

mechanical properties has been demonstrated for aluminum alloys »'' and<br />

other materials (8)# in cases where grain boundary scattering is dominant,<br />

various models (l>°,10) offering good agreement with experiment can be used<br />

to calculate the grain size from the frequency dependence of attenuation. The<br />

ultrasonically measured grain size, 6, can then be correlated with mechanical<br />

properties via the use of the Hall-Petch relationship.<br />

U = uo + kS-i (1)<br />

where M is the mechanical property of interest, n, is a constant dependent<br />

on composition, and k is a proportionality constant. This latter approach was<br />

used by Klinman et al (11) to successfully predict yield strength, tensile<br />

strength and DBTT's in carbon steels of known compositions. Another approach<br />

was taken by A. Vary ("), who suggested an empirical relation relating<br />

fracture toughness, K.ic, yield strength oy, and ultrasonic attenuation:<br />

Klc 2 /Oy = 8.12 x 10 6 (Va&j) 0 ' 31 " 1 (2)<br />

where V£ is the velocity of longitudinal waves in the material and ßg is<br />

the slope of the attenuation versus frequency curve at a frequency, f =<br />

Vg/6, where the wavelength is equal to the grain size. Since f is<br />

generally outside the range of most normal attenuation measurements (eg. f =<br />

0.5 GHz in steel with 6 = 10 Mm), the value of fJ$ is extrapolated from<br />

measurements in the 10 to 50 MHz range. Two ma rag ing steels and a titanium<br />

alloy, aged at various temperatures, were found to obey relation (2).<br />

However, studies on Fe-C alloys (13) have shown that increasing the grain<br />

size or increasing the cabon content, both cause an increase on the DBTT but<br />

have opposite effects on ultrasonic attenuation. This is attributed either to<br />

diminished absorption due to an increase in dislocation damping with<br />

increasing C content, or to diminished scattering due to a decrease of elastic<br />

anisotropy of the grains related to the presence of pearlite or cementite<br />

around the ferritic grain boundaries. Thus it is difficult to isolate one<br />

component of the ultrasonic attenuation, and in particular, to differentiate<br />

between absorption and scattering. It is also difficult to vary one material<br />

property such as fracture toughness while others remain constant.<br />

In the present study, this is accomplished by correlating the ultrasonic<br />

behavior and mechanical properties of a 403 stainless steel between -60 and<br />

+40°C. In this temperature range, the plain strain fracture toughness, Kjc,<br />

changes by =250% because of a smooth brittle to ductile transition, while<br />

composition and microstructure remain unchanged.

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