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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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281 -<br />

Finally, resonances of saw-cut balls were practically undamped compared<br />

to those of naturally cracked balls. Evidently the latter are damped by<br />

friction occuring along the crack interface. Consequently, one can also<br />

assume that the shear motion depicted in Fig.5 for the "shear" mode is<br />

unlikely to occur in naturally cracked balls.<br />

2. DEVELOPMENT OF AN ACODSTIC CRACK DETECTOR FOR SORTING GRINDER BALLS<br />

Principle of operation<br />

We have seen that noticeable differences exist between the sound<br />

produced by the impact of uncracked grinder balls and the sound produced by<br />

the impact of cracked ones. From this, it was concluded that a device that<br />

would use these differences to acoustically detect and sort out the cracked<br />

grinder balls from the good ones was technically feasible and a laboratory<br />

scale prototype was developed. Figure 6 is a photograph of the device. The<br />

mechanical assembly allows the balls to drop from a constant height on a<br />

fixed anvil. It is composed mainly of 4" PVC tubing supported by a bolted<br />

"Dexion" frame. The anvil is a 2" steel cube mounted in a foam filled box.<br />

A 6" long aluminium rod mounted on a hinge inside the horizontal sorting<br />

tube and activated by a solenoid deflects the cracked balls toward the first<br />

opening, while the others exit by the end opening.<br />

The impact sound is picked up by a nearby microphone and electronically<br />

analyzed. The ball finally exits by one of two ports depending on whether<br />

or not a crack has been detected. The electronic circuit "listens" for<br />

those mid-range resonances typical of cracked grinder ball impacts that<br />

immediately follow the initial pulse. It measures the "amount" of such<br />

resonances and uses it as a criterion to decide whether the ball is good or<br />

bad. Figure 7 is a simplified diagram of the circuit. The microphone is a<br />

Bruel & Kjaer i" microphone and power supply flat to 30 kHz. It is located<br />

in the target area, as near as possible to the trajectory of the grinder<br />

balls, positioned downwards to prevent any buildup of dust or other<br />

pollutants on its membrane. The detector consists of a band pass filter<br />

(10-20 kHz), a rectifier and a gated integrator. The output voltage thus<br />

represents the amount of acoustic energy between 10 and 20 kHz integrated<br />

over the time window defined by a gate signal. It is compared to a<br />

reference voltage to determine whether the ball is cracked or not. The<br />

logic block carries out the measurement sequence. It uses the "initial<br />

pulse" as a trigger event, resets the integrator and holds it on reset for<br />

about 1 ms. This adjustable delay determines the start of the time window<br />

and allows the blanking out of the initial pulse. It then frees the<br />

integrator for about 10 ms and then interrupts the integration. This<br />

defines the width of the time window, the end of which is positionned just<br />

before the occurence of a second collision due to the recoil of the anvil<br />

bouncing back on the grinder ball. While the time window is open, the<br />

output of the integrator is compared to an adjustable reference and the<br />

output of the comparator commands the operation of the sorting device. As<br />

the time window closes, the trigger of the logic block is disabled for about<br />

100 ms to prevent retriggering on the second collision mentionned above or<br />

any other spurious noises. After that delay, it is ready to be retriggered<br />

when an other ball hits the anvil. Until then, the integrator is on hold,

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