17.06.2013 Views

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

- 213 -<br />

6. The axial gap profile should be similar when computed<br />

using either end of the pressure tube as a reference.<br />

Note that if the gap at both ends of the pressure tube<br />

are not equal to 8 mm, repeating the calculations using<br />

the other end as a reference will not just shift the gap<br />

profile by the difference. The shape of the profile will<br />

also change due to the non-linearity in the data base.<br />

The accuracy of the gap measurements is primarily determined by the effect of<br />

the ±0.05 mm uncertainty in the wall thickness measurements at both the<br />

reference and measurement points. Referring to Figure 3, the uncertainty in<br />

the location of the reference point, which must be located along the line of<br />

constant 8 mm gap for axial scans, can also be expressed in terms of the eddy<br />

current signal voltage as approximately ± 0.08V. Doing so allows the<br />

uncertainty to be transferred to the measurement point and to consider the<br />

reference point fixed. The additional uncertainty in the measurement point<br />

due to its associated wall thickness measurement can also be expressed in<br />

terms of the eddy current signal, but the exact conversion factor will depend<br />

on the size of the gap. The wall thickness measurements can be assumed to be<br />

indépendant and normally distributed and so both of the uncertainties in the<br />

measurement point may be combined as the square root of the sum of the<br />

squares. The result will vary from a high of +0.11V for a gap of 8 mm to a<br />

low of +0.083V for a gap of 0 mm. An error bound of ±(30% + 0.1 mm) on<br />

computed gap values approximates this overall uncertainty and is the magnitude<br />

of the error bars that have been placed around the sample results in Figure<br />

10.<br />

S. AKEAS ft» DEVELOPMENT<br />

The field experience in Pickering has served to solidify the gap measurement<br />

procedure and also to uncover various weak points in the equipment which<br />

effect the results. Further development is being done using the CIGAR<br />

inspection system with the emphasis on Zr-2.5%Nb pressure tubes now that the<br />

Zircaloy-II tubes in Pickering Units 1 and 2 are to be replaced.<br />

The use of the CIGAR inspection system addresses a number of equipment<br />

reliability problems encountered in Pickering which made it difficult to<br />

isolate and solve problems originating with the measurement technique. The<br />

most important advancement is that both the eddy current and wall thickness<br />

data are collected automatically during the same axial scan. This ensures the<br />

proper alignment of both probes and enables a large amount of data to be<br />

collected which can then be smoothed, reducing any unbiased error in the<br />

individual measurements. Another improvement is the gentler and largely<br />

automatic handling of the signal cables and their connections which has<br />

resulted thus far in stable and reliable eddy current signals. Very promising<br />

and repeatable results have been obtained to date but more testing is still<br />

required. Some development work still remains to be done in the area of<br />

pressure tube resistivity variations and in the quality of the eddy current<br />

probe, both in terms of its temperature sensitivity and its consistency in<br />

manufacture.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!