A CONTRIBUTION TO QUANTIFYING THE SOURCES OF ERRORS IN PAUT

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A CONTRIBUTION TO QUANTIFYING THE SOURCES OF ERRORS IN PAUT Tim Armitt, Lavender Int. NDT Consultancy Services Ltd, UK Peter Ciorau, Tetra Tech Energy Division, Canada Jason Coulas, Ontario Power Generation, Canada ABSTRACT: The paper presents specific examples of PAUT errors for location and crack sizing. The errors are grouped based on equipment capabilities/limitations and test piece / flaw characteristics / inspection conditions. The following parameters were taken into consideration: wedge velocity, wedge angle, element pitch, the number of points quantity / A-scan, angular resolution and element resolution for a VPA. Examples of error location are given for different weld inspections scenarios. Recommendations are made for field application to reduce the error value in flaw location and sizing. The paper results concluded: the tolerances on above mentioned variables are very tight ( at the limit of PAUT lab conditions) for a crack height and location (index) error of ± 0.5 mm. Introduction PAUT basics principles and performance assessment fulfill the laws of ultrasounds. The detection and sizing capabilities depend on specific parameters, similar to conventional UT (ref.1-2). The S-scan display myth led to the idea the PAUT is an ideal NDT tool: what you see is what the flaw is looking like in the test piece (see Figure 1 as an example). Courtesy: OlympusNDT, USA) Figure 1: Examples of PAUT S-scan displays and defect confirmation by MP and optical methods. The PAUT results from Figure 1 are due to a high-reliability process (redundancy, diversity and validation), in combination with very tight tolerances on probe parameters, set-ups and data analysis (ref.3). PAUT is a computer-driven technology and the possibility to make a mistake in the set-up or to scan with a worn wedge may lead to errors in detection, location and sizing. During the last decade specific literature and standards were published dealing with different PAUT aspects of essential variables (probe, wedge, machine, set-up, scanner characteristics, data acquisition) (ref.4-19). The main conclusions from these papers are: PAUT method is subject to systematic and random errors; tolerances shall be set based on application requirements regarding the flaw characteristics; there is no published data about tolerances on essential variables and different levels of errors for crack height measurement. The present paper is dealing with specific aspects of quantitative errors in location and sizing of fatigue cracks and systematic errors due to number of sampling points / A-scan. The paper will detail the following topics related to tolerances assessment for a specific error value (0.5 mm and 1.0 mm) in sizing (height) and positioning (index): - the sweep resolution - the VPA resolution - the number of sampling points - the wedge velocity - the wedge angle - the probe pitch 1

Errors due to Angular Resolution, Number of Sampling Points and VPA Resolution The S-scan displays PAUT data on the following axis: horizontal-index, vertical-depth. The errors in location and height are based on small angular increments and the number of effective sampling points on A-scan (see Figure 2 to Figure 4). Figure 2: Precision in location dependence on UT path, refracted angle and angular resolution. Figure 3: Principle of over-all precision location based on interpolation of data between two storage points on each A-scan. Figure 4: Example of distance between two storage points for three inspection scenarios and points quantity. An example of error assessment for index and height is presented in Figure 5. The error could be reduced by a factor of 4 if the number of stored points is increasing from 160 to 640. Using the scale factor or compression rate, may speed-up the acquisition of a smaller file size, but has a negative effect on location and sizing. 2

Figure 5: Example of error assessment for PAUT inspection scenarios of a 100-mm thick weld for an UT path of 292 mm at 60 for a PAUT probe of 4 MHz, 1-mm pitch. Angular resolution has effect on pixel size, image quality and crack height measurement. Figure 6 presents an example from ref.7. The crack pattern for angular resolution of 4 is no longer correctly displayed. Angular resolution shall be 1 for a proper display and height sizing. Figure 6: Example of crack height measurement at different angular resolution. Electronic scanning at fixed refracted angle is performed by grouping a number of elements and moving the VPA along the active aperture with a specific resolution. Figure 7 to Figure 9 illustrate the errors associated with effective VPA and number of sampling points/a-scan. It is obvious the errors are reduced for larger number of points (640) and for a 1-element movement of VPA over the selective active area. Figure 7: Variation of index and height due to sweeping step across the active aperture. 3

Figure 8: Example of index and height variation errors dependence on element step for a 5-MHz 16-element, pitch 0.6 mm; probe angle of incidence = 39. Figure 9: Dependence of index and height errors on points quantity / A-scan. Errors of 0.5 mm for height and 1 mm for index are achievable for point quantity of 320 and higher. Errors Due to Probe and Wedge Features Extensive studies were performed by OPG during 2004-2011 intervals. Software simulation and actual probe interchange were used to set tolerances on specific variables. Some of the results were published in ref. 6-7. A new evaluation of some of the published data related to crack location and height accuracy measurement is presented in Figure 10 to Figure 14. 4

Figure 10: Example of crack height accuracy dependence on wedge velocity. Probe of 6 MHz-16 elements on 47 Plexiglas wedge. Software simulation using the focal law set-up. Figure 11: Example of crack height accuracy dependence on wedge angle. Probe of 6 MHz-16 elements on 47 Plexiglas wedge. Software simulation using the focal law set-up. Figure 12: Example of crack height accuracy dependence on probe pitch size; probe of 6 MHz-25 elements- 0.4 mm pitch on Plexiglas wedge of 37. Software simulation using the focal law set-up. 5

Figure 13: Example of crack location accuracy dependence on probe pitch size; probe of 6 MHz-25 elements- 0.4 mm pitch on Plexiglas wedge of 37. Software simulation using the focal law set-up. Conclusions The data presented in this paper conclude: - Smaller value for angular resolution ( θ=0.5 ) and for VPA (0.5 or 1 element) will lead to errors = 0.5 mm; - 0.5 mm error on both axis (index and depth) is the best of PAUT and very tight to keep - Quantity points along an A-scan stored and analyzed is an essential variable for error assessment. An error of 0.5 mm for height and 1 mm for index is achievable for n > 320 points / A-scan. - Pitch tolerance of 25 µm for a 0.5-mm error in location and sizing is a challenge value for probe manufacturer - Height and index errors depend on refracted angle. If the independent events are combined in different scenarios, the over-all error is increasing from an ideal ± 0.5 mm to ± 1.1 mm (see Figure 14). Figure 14: Example of error trend due to independent events, such as point quantity, angular resolution, wedge angle, wedge velocity, and probe pitch tolerances. 6

References 1. CEGB OED/STN/87/20137: CEGB Code of Practice for Ultrasonic Measurement Errors Assessment -CEGB-UK, May 1987 2. Ciorau, P.: Random and systematic factors affecting peak amplitude level in ultrasonic inspection of welded joints" - Canadian Journal of NDT, vol. 17, no.3, 1995, pp. 14-20.; Doc. IIW-Vc-923-97/OE 3. Ciorau, P., Pullia, L.: How Reliable is Your Call? OPG Phased Array Ultrasonic Inspection Experience on Siemens- Parson Turbine Blade Roots 2001-2007 - ndt.net vol. 12, no. 6 (June 2007) / Proceedings 10-th EPRI Turbine Workshop-Phoenix-Aug.13-15-2007 4. Cameron, N. Probe and wedge characterization; acceptance criteria. Proceedings, 3rd Phased Array Inspection Seminar, Seattle, USA, 2003. 5. EPRI white paper:. Cancre, F., and M. Dennis. Effect of the Number of Damaged Elements on the Performance of an Array Probe., EPRI, USA 2001 6. OlympusNDT: Advances in Phased Array Ultrasonic Technology Applications -editors: N.Dubé and M. Moles, Waltham, USA, 2007, chapter 5.2 7. Poguet, J., Ciorau,P. : The Influence of PAUT Parameters on Crack Height, Location and Pattern Proceedings 8 th Int. Nucl. NDE Conf.-paper Th. 3.B.2.- Berlin-Sep 2010; 3 rd COG- CINDE ISI Conf-Markham-June 2010; ndt.net, vol.15, no.12-dec. 2010 (with ppt) 8. Armitt,T.: Phased Array not the Answer to Every Application - Proceedings ECNDT, paper We3.1.3-Berlin, Sep-2006; ndt.net no.11-2006 9. Ciorau, P., Poguet, J., Fleury, G.: Reproducibility and Repeatability of NDT Phased Array Probes Proceeding 3 rd EPRI PA Seminar, Seattle, June 2003 10. Ciorau, P., Poguet, J., Fleury, G.: A Practical Proposal for Designing, Testing and Certification Phased Array Probes Used in Nuclear Applications. 4 th Int. NDE Conf. Nuclear, London, Dec, 2004 11. Ciorau, P.: A novel checking technique for probe characterization and phased array system performance assessment, ndt.net vol.12, no.6 (June 2007) 12. Ciorau, P.: Phased Array Equipment Substitution-Practitioner Approach for Large-Scale Turbine Inspection - ndt.net- vol. 12, no.6 (June 2007) 13. Armitt,T.: Measurement and sizing capabilities of PA applications -Lavender Int. Consultancy API training course-module 2-Houston-USA, 2011 (not for distribution) 14. ASTM vol. 03.03-2011: Standard Guide-Evaluating Performance Characteristics of Phased- Array Ultrasonic Examination Instruments and Systems, ASTM E 2491-06 15. ASTM vol. 03.03-2011: Practice for Contact Ultrasonic Testing of Welds Using Phased Arrays ASTM E 2700-09 16. ASME V: Case 2541 - Use of Manual Phased Array Ultrasonic Examination 2010 17. ASME V: Case 2557 Use of Manual Phased Array S-Scan Ultrasonic Examination Per Article 4 Section V - 2010 18. ASME V: Case 2558 Use of Manual Phased Array E-Scan Ultrasonic Examination Per Article 4 Section V 2010 19. EPRI: Nondestructive Evaluation: Procedure for Manual Phased Array Ultrasonic Testing of Piping EPRI Report 1016650-Aug.2008 ACKNOWLEDGEMENTS The authors wish to thank the following organizations and people: OPG-IMS Management, Canada and Lavender Int. NDT Consultancy Services, UK for granting the publication of this paper OlympusNDT, USA for allowing to use five figures from their published book (ref.6) 7