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IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research

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IGC<br />

<strong>Annual</strong> <strong>Report</strong> 2007<br />

Table 1 : Relative comparison of sensitiveness of different NDE techniques <strong>for</strong><br />

characterization of ageing behaviour in maraging steel<br />

N-Non sensitive<br />

YY-More sensitive<br />

complimentary in<strong>for</strong>mation or<br />

confirming the observation of<br />

other techniques, this enhances<br />

the use of multiple techniques<br />

and adopting multi-parametric<br />

approaches is very attractive<br />

and is expected to enable very<br />

effective characterization of<br />

microstructures. In this study,<br />

NDE parameters such as<br />

ultrasonic velocity, magnetic<br />

Barkhausen emission (MBE)<br />

RMS voltage, eddy current (EC)<br />

Fig.1 Variation in hardness,<br />

ultrasonic wave velocity, and<br />

positron annihilation life time<br />

parameter with aging at 755 K.<br />

impedance magnitude,<br />

positron life-time and X-ray<br />

diffraction based austenite<br />

volume fraction have been<br />

employed to develop a<br />

comprehensive<br />

NDE<br />

Y-Sensitive<br />

Y?-Sensitive but requries precise measurements<br />

methodology<br />

<strong>for</strong><br />

characterization of ageing<br />

behaviour of M250 grade<br />

maraging steel aged at 755 K<br />

<strong>for</strong> different durations.<br />

The variations in hardness,<br />

ultrasonic longitudinal wave<br />

velocity and positron<br />

annihilation life time with aging<br />

duration are shown in Fig.1.<br />

The variations in hardness,<br />

MBE rms voltage, volume % of<br />

austenite (XRD based) and<br />

impedance amplitude with<br />

aging duration are shown in<br />

Fig.2. Ultrasonic velocity<br />

showed good promise in<br />

characterizing the intermetallic<br />

precipitation process and was<br />

able to pick up the austenite<br />

in<strong>for</strong>mation to some extent. Its<br />

drawback is with respect to<br />

obtaining any in<strong>for</strong>mation<br />

about the defect structure and<br />

early detection of initiation of<br />

austenite reversion. Hence, this<br />

technique is found to be very<br />

sensitive to monitor only the<br />

intermetallic precipitation<br />

behaviour. Positron annihilation<br />

studies were found to be very<br />

sensitive to changes in defect<br />

structure during initial aging<br />

and precipitation to some<br />

extent. Fig.3 shows the bright<br />

field TEM image of defects<br />

(dislocations) in solution<br />

annealed condition. The<br />

austenite reversion has<br />

insignificant effect on positron<br />

annihilation parameter. Hence,<br />

this technique can be used <strong>for</strong><br />

high sensitive characterization<br />

of defects such as vacancies or<br />

dislocations. MBE study showed<br />

good promise in identifying the<br />

non-magnetic austenite phase<br />

compared to the intermetallic<br />

precipitation and defect<br />

structure. EC technique had<br />

shown good promise in<br />

characterizing the austenitic<br />

reversion ahead of ultrasonic<br />

and almost on par with MBE.<br />

As this technique is more<br />

amenable to shop floor, it can<br />

be used <strong>for</strong> quick and reliable<br />

determination of volume % of<br />

austenite on shop floor as well<br />

as on components. The bright<br />

field TEM image showing<br />

Fig.1 Variation in hardness, MBE rms<br />

voltage, EC amplitude and<br />

volume % of austenite determined<br />

by XRD with aging at 755 K.<br />

120 ENABLING TECHNOLOGIES

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