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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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- 358 -<br />

The impedance (or the phase lag) of each coil is measured and if<br />

there is a sufficiently large deviation from the measurement<br />

above a good test object a 1 is assigned to the location of the<br />

coil in question. Another approach has the coils acting<br />

simultaneously- as driver and receiver. The induced eddy currents<br />

would be similar around each probe. If the eddy current signal<br />

could be analysed at the coil location for depth (by measuring<br />

amplitude and phase at frequencies), an immediate profile of<br />

the defect could be shown. A holographic method of imaging is<br />

also possible in the AS mode. It is assumed that the response of<br />

a coil is not altered by the presence of neighbours. If no<br />

reasonable pictures can be developed from the static case (AS),<br />

it will be difficult to develop these from the dynamic case (AD).<br />

There are similarities with early radiographie techniques<br />

indicating the presence of something but no indication of the<br />

depth. Therefore a binary picture will not give the necessary<br />

information to fully evaluate the importance of a defect.<br />

However, it suffices for the detection of anomalies.<br />

In our approach, the response of each individual coil is<br />

processed, resulting in a depth profile. The experiments<br />

addressed the questions below.<br />

- Are all the coils identical or can their response be made<br />

identical?<br />

- Are neighbours altering the coil response?<br />

- Can a calibration curve be drawn for all probes?<br />

EXPERIMENTAL<br />

Design of Coils and Building of the Array<br />

We used the Hocking Phasec D6A Eddy Current instrument, which is<br />

a multi-frequency device (ranging from 1 kHz to 1 MHz), highly<br />

flexible and easy to operate. The Hocking Phasec D6A prefers<br />

driver coils with impedances larger than 50 ohms. This puts<br />

certain limitations on the choice of coils and the working<br />

frequency.<br />

Two tools assisted in coil design. The first is a computer<br />

program AIRCO, developed by Dodd et al.,(9) which allows for the<br />

calculation of the impedance of coils with air cores, taking<br />

into account geometry and wire gage. This program was adapted<br />

for the microcomputer in C BASIC. Ferrite cores were also<br />

introduced to increase the inductance of the coils.<br />

Probes were manufactured in-house or were commissioned from a<br />

reputable manufacturer for the final array. An HP 4192A<br />

impedance meter was used to measure the impedance and inductance<br />

of the coil in air. The resonance frequency of the coils was over<br />

600 kHz.

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