EPJ Nuclear Sci. Technol. 1, 4 (2015)© N. Kobayashi et al., published by EDP Sciences, 2015DOI: 10.1051/epjn/e2015-50043-1

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Eddy current testing system for bottom mountedinstrumentation weldsNoriyasu Kobayashi1*, Souichi Ueno1, Naotaka Suganuma1, Tatsuya Oodake2, Takeshi Maehara3, Takashi Kasuya3,and Hiroya Ichikawa4

1 Power and Industrial Systems Research and Development Center, Toshiba Corporation, 8, Shinsugita-cho, Isogo-ku, Yokohama235-8523, Japan

2 Power and Industrial Systems Research and Development Center, Toshiba Corporation, 1, Komukaitoshiba-cho, Saiwai-ku,Kawasaki 212-8581, Japan

3 Keihin Product Operations, Toshiba Corporation, 2-4, Suehiro-cho, Tsurumi-ku, Yokohama 230-0045, Japan4 Isogo Nuclear Engineering Center, Toshiba Corporation, 8, Shinsugita-cho, Isogo-ku, Yokohama 235-8523, Japan

*e-mail: no

This is an O

Received: 19 June 2015 / Received in final form: 18 August 2015 / Accepted: 27 August 2015Published online: 05 December 2015

Abstract. The capability of eddy current testing (ECT) for the bottom mounted instrumentation (BMI) weldarea of reactor vessel in a pressurized water reactor was demonstrated by the developed ECT system andprocedure. It is difficult to position and move the probe on the BMI weld area because the area has complexlycurved surfaces. The space coordinates and the normal vectors at the scanning points were calculated as thescanning trajectory of probe based on the measured results of surface shape on the BMI mock-up. The multi-axisrobot was used to move the probe on the mock-up. Each motion-axis position of the robot corresponding to eachscanning point was calculated by the inverse kinematic algorithm. In the mock-up test, the probe was properlycontacted with most of the weld surfaces. The artificial stress corrosion cracking of approximately 6 mm in lengthand the electrical-discharge machining slit of 0.5 mm in length, 1 mm in depth and 0.2 mm in width given on theweld surface were detected. From the probe output voltage, it was estimated that the average probe tilt angle onthe surface under scanning was 2.6°.

1 Introduction

Eddy current testing (ECT) techniques to detect a defect,especially a stress corrosion cracking (SCC), on a reactorvessel (RV) and reactor internals have been developed as oneof the surface inspection methods for nuclear power plants[1–7]. As a part of maintenance methods for the RV andreactor internals, laser peening and underwater laser beamwelding techniques to prevent and repair from the SCC havebeen developed [8–11]. These inspection and maintenancetechniques can contribute to shorten their work period,including the initial set-up because it is possible to workunderwater without draining the reactor coolant. In order toprovide faster services, the defect detection capability of theECT probe using the cross coil has been estimated for theinspection before and/or after the underwater laser beamwelding for thedissimilarmetalweldingareaat theRVnozzlein pressurized water reactors (PWRs) [12–14]. The ECT

riyasu.kobayashi@toshiba.co.jp

pen Access article distributed under the terms of the Creative Comwhich permits unrestricted use, distribution, and reproduction

system, including the smallECTprobeandtheprobemovingequipment based on the portable laser peening system, hasbeen developed for the bottom mounted instrumentation(BMI)weld area inPWRs [15]. In this development, the SCCdetection capability of the system was demonstrated bymoving the probe on the area of 10mm� 6mm of the BMImock-up [15].

More precise probe action control is required to movethe probe on the whole BMI weld area because the area hascomplexly curved surface and the narrow spaces. Wemeasured the surface shape of weld area using the laserdisplacement meter and made the scanning trajectory ofthe probe based on the shape measurement data of thecomplex surface. As a BMI mock-up test, the ECT probewas automatically moved on the whole BMI weld area bythe multi-axis robot. From the test results, we evaluatedthe defect detection capability of the ECT system and theprobe tilt angle on the weld surface under scanning. In thispaper, we describe the procedure of BMI mock-up test; theresults of measuring weld surface shape and defectdetection tests.

mons Attribution License (http://creativecommons.org/licenses/by/4.0),in any medium, provided the original work is properly cited.

Fig. 1. Process flow diagram of ECT for BMI welds.

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2 Weld surface shape measurement

2.1 Procedure of BMI mock-up test

A process flow diagram of an ECT for BMI welds is shownin Figure 1. The three-dimensional shape of inspected weldsurface was measured in order to generate the precisescanning trajectory of ECT probe. After generating thetrajectory, the action of multi-axis robot, which moves theprobe along the scanning trajectory on the weld surface,was planned and checked for the interference between therobot and the BMI mock-up. The probe was moved on thewhole BMI weld area by the robot to acquire the ECTdefect detection data. Finally, we analyzed the acquireddata, including the signal processing for noise rejection andsignal identification.

Fig. 2. Measurement of weld su

2.2 Measurement of surface shape

We measured the surface shape of the weld area on theBMI mock-up for generating the scanning trajectory ofECT probe. A half of weld area was the target for scanningby the ECT probe because the mock-up is axisymmetric.The measurement range of surface shape is the half side ofweld area and within approximately 60 mm in radiuscentering on the BMI nozzle as shown in Figure 2. Thesensor head of laser displacement meter (KEYENCE,LJ-G200) mounted on the multi-axis robot measured thethree-dimensional surface shape in an approximately0.5 mm interval at the points of approximately 60 mmfrom the center of nozzle within the measurement range.The sensor head rotated round trip half side around thenozzle. The laser spot size is 180 mm� 70 mm. The basework distance is 200 ± 48 mm.

2.3 Scanning trajectory of probe

The space coordinates and the normal vectors at the scanningpoints as the scanning trajectory of ECTprobe onwelds weregeneratedbasedonthemeasured results ofweld surface shapeon the BMImock-up. The calculated results of the trajectorywere shown in Figure 3. The blue range in Figure 3 is themeasured surface shape. The red arrows indicate thecalculated results of normal vector for determining the probeangles at the scanning points. The probe is set on theinspected surface, as the probe central axis is adjusted tocoincide with the normal vector at each scanning point.

2.4 Multi-axis robot

The multi-axis robot, which moves the ECT probe, isshown in Figure 4. The robot has three translation axes and

rface shape on BMI mock-up.

Fig. 3. Scanning trajectory of ECT probe.

N. Kobayashi et al.: EPJ Nuclear Sci. Technol. 1, 4 (2015) 3

four rotation axes. The probe was mounted on the end ofthe robot arm. Each motion axis position as a robot actioncorresponding to each scanning point was calculated by theinverse kinematic algorithm. After the two rotating motionaxis positions were provided as the constant values, theother motion axis positions were led in the calculation. Theprobe-scanning trajectory shown in Figure 3 was dividedinto the three ranges (nozzle, J-welds and build-up welds)

Fig. 4. Multi-axis robot.

as shown in Figure 5. The three different algorithms for thethree ranges were used to prevent from the interferencebetween the robot and the BMI mock-up. It was confirmednot to interfere between the robot and the mock-up usingthe three-dimensional simulator before the mock-up test.

3 Experimental apparatus and methods

3.1 ECT system

A block diagram of the ECT system is shown in Figure 6.This system consists of the ECT probe, the multi-axisrobot, the robot controller, the ECT data acquisitionsystem and the ECT data analysis system. The probe wasmoved to a start point of scanning manually. As soon as ascanning was started under the order from the robotcontroller, the ECT data acquisition system received thecoordinate data of the start point from the controller andvoltage signals from the probe. After the acquisition systempaired the coordinate data with the voltage signals andsaved them into a memory, the acquisition system sent anacquisition end signal at the start point to the controller.The controller automatically moved the probe to the nextscanning point using the multi-axis robot based on theprobe-scanning trajectory. Thesemovements were repeateduntil the entire scanning is completed. The ECT dataanalysis system read the scanning coordinate data and theprobe output signals, and conducted the signal processingand displayed the inspected results.

3.2 BMI mock-up and scanning range

A schematic of the BMI mock-up simulating the outermostnozzle at the bottom of RV is shown in Figure 7 [15]. Thenozzle was fixed to the bottom of RV by a tungsten inert gas

Fig. 5. Divided scanning trajectories.

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(TIG) welding. The surface of weld area was machinedsmoothly. Both the nozzle and the weld metal are made ofalloy 600. Artificial and circumferential defects were givenon the weld surface at the points of 10 mm from the outersurface of nozzle. The type and size of defects are describedin Table 1. It was defined that the top of themock-up is at 0°in circumferential angle as shown in Figure 7. The length ofSCC shown in Table 1 is the value of indication onpenetrant testing (PT).

The scanning range by the ECT probe is shown inFigure 8. The start point of scanning is on the outer surfaceof nozzle at 0° in circumferential angle and approximately3 mm above the J-weld. The probe was moved in less than0.5 mm interval within the scanning range in a circumfer-ential direction and made several round trips half sidearound the nozzle. An end point of scanning is on the build-up weld surface at 0° in circumferential angle andapproximately 40 mm from the center of nozzle. Thisscanning range includes the nozzle, the J-welds, the build-up welds and the artificial defects.

3.3 Experimental and calibrating conditions

The experimental and calibrating conditions are shownin Table 2. We used the developed ECT probe [15] thathas small-sized cross coil and the higher directional

Fig. 6. Block diagram of ECT system.

characteristics of magnetic field in the mock-up test. Thediameter of the probe tip that has contact with an inspectedsurface is 3.4 mm. The probe operated with the differentialmode at the frequency of 250 kHz, 500 kHz and 1MHz. Thecalibration block made of alloy 600 has an EDM slit of80 mm in length, 1 mm in depth and 0.3 mm in width. Thethickness of calibration block is 20 mm. We calibrated theoutput voltage and the phase angle to 2 V and 90° using thisblock in air, respectively.

4 Experimental results of mock-up test

The C scope images as seen through the signal processingfor the absolute values of imaginary part of ECT outputvoltages at a frequency of 250 kHz, 500 kHz and 1MHz areshown in Figure 9. At a frequency of 250 kHz, the clearsignals from the defect A (SCC), the defect B (EDM) andthe defect C (EDM) were confirmed. It was considered thatthe signals from the defect D (EDM) and the defect E(SCC) were not detected because the volumes of the defectD and the defect E are smaller than those of the other

Fig. 7. Schematic of BMI mock-up [15].

Table 1. Artificial defects.

Defect Type Length (mm) Depth (mm) Width (mm)

A SCC Approx. 6 No data No dataB EDM slit 0.5 1.5 0.2C EDM slit 0.5 1.0 0.2D EDM slit 0.3 1.0 0.2E SCC Approx. 3 No data No data

EDM: electrical-discharge machining; Approx.: approxi-mately.

Table 2. Experimental and calibrating conditions.

ECT probe Cross coil

Operation mode DifferentialFrequency (kHz) 250, 500, 1000Atmosphere In airCalibration block Alloy 600 (20 mm in thickness)EDM slitLength (mm) 80Depth (mm) 1Width (mm) 0.3CalibratedOutput voltage (V) 2Phase angle (°) 90

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defects. The maximum output voltages of the detecteddefects were 0.93 V in the defect A, 0.33 V in the defect Band 0.24 V in the defect C. The ratio of maximum outputvoltages between the defects B and C was 1.4. This valuewas roughly equal to the ratio of the volumes between thedefects B and C (1.5). On the other hand, the maximumoutput voltage of the noises was 0.25 V. Under the followingthree assumptions:

a.

the maximum output voltage from the defect isproportional to the defect volume;

b.

the criterion for defect detection is that the signal tonoise ratio is more than 2;

c.

the ECT can detect the defect of 0.5 mm and more indepth,

it is estimated that the minimum EDM slit size that thisECT system can detect is approximately 2.3 mm in length,0.5 mm in depth and 0.2 mm in width. The output voltageof the defect E was less than 0.125 V. It was difficult torecognize the figure of the defect E visually. If the width ofthe defect E was 0.05 mm, it is evaluated using the aboveassumption (a) that the depth of the defect E is less than0.38 mm. Although the length of the defect E is longer thanthe lengths of the other EDM slits, it is considered that thesignal from the defect Ewas not detected because thewidthand depth are smaller than those of the other EDM slits.

Fig. 8. ECT sc

The noises increased at higher frequencies. It wasconsidered that the sensitivity of ECT probe for the changeof surface shape was increased by the dense eddy current onthe mock-up surface layer because of shallower skin depthsat higher frequencies. The skin depth of alloy 600 at eachfrequency is shown in Table 3. The skin depth at eachfrequency is the same or less than the depth of the EDM slitgiven on the calibration block, 1.0 mm. When a defectdepth is the same or more than 1.0 mm, a phase angle of asignal from a defect indicates the near-calibrated value,approximately 90° or �90°. Positive and negative valuesmean that directions of defects are mutually orthogonal. Aphase angle of an eddy current lags to the direction ofmaterial depth [16]. Therefore, a phase angle of a signalfrom a defect may lag behind the calibrated value if a defectdepth is less than 1.0 mm. The measured phase angles of thesignals from the defects (A, B and C) and the noises (F, Gand H) in Figure 9 are shown in Table 4. It was reasonablethat the phase angles of the signals from the defects A, Band C were approximately 90° or �90°. It was consideredthat the noises F and G were caused by the change of

anning range.

Fig. 9. C scope images of ECT output voltages.

Table 4. Measured phase angles.

Frequency (kHz) 250 500 1000Phase angle (°)Defect A 99 91 80Defect B 103 100 88Defect C 90 87 83Noise F 98 90 83Noise G �95 �94 �112Noise H Out of measure �160 �105

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surface shape more than 1.0 mm in depth because theirphase angles were approximately 90° or �90° as in the caseof the defects A, B and C. The phase angle of noise H at thefrequency of 500 kHz was largely lagging behind �90°. Itwas considered that the phase lag was observed at thefrequency of 500 kHz having the deeper skin depth becausethe depth of the surface shape change was much less than1.0 mm. Themaximum output voltages from the defects areroughly equal at each frequency. It was estimated that thebest frequency for the defect detection by the used ECTprobe in this BMI mock-up test is 250 kHz.

5 Discussions

5.1 Relationship between probe tilt angle and outputvoltage of single coil

Because the probe tilt angle on the inspected surfaceinfluences a defect detection capability, the tilt angle under

Table 3. Skin depth of alloy 600 at each frequency.

Frequency (kHz) 250 500 1000Skin depth (mm) 1.0 0.71 0.50

scanning in this mock-up test could be roughly estimated.First of all, we investigated the relationship between theprobe tilt angle on the flat surface specimen and the outputvoltage of single coil. The single coil means one of two coilsthat compose the cross coil and is more sensitive for theprobe tilt angle than the differential mode of cross coil usingthe two coils. The area without the EDM slit of thecalibration block shown in Table 2 was used as a flat surfacespecimen in this measurement. We defined the meaning ofthe probe tilt direction and angle as shown in Figure 10,respectively.

The measured result of the relationship between theprobe tilt direction and the output voltage of single coil at afrequency of 500 kHz is shown in Figure 11. The measuredresult at a frequency of 500 kHz provided the smallestoutput voltage variation in the prior confirmation. The tiltangle is 9° at constant angle. The output voltage wasnormalized by the value at the tilt direction of 0° becausethe sensitivity of the ECT data acquisition system in thismeasurement was different from that in the mock-up test.The output voltage was constant within the variation of15% by a change in the tilt direction. We measured the

Fig. 10. Probe tilt direction and angle.

Fig. 11. Relationship between probe tilt direction and outputvoltage of single coil.

Fig. 13. Estimated probe tilt angles under scanning on J-welds ofBMI mock-up.

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relationship between the probe tilt angle and the outputvoltage of single coil under the condition of 0° in probe tiltdirection. The sensitivity of the ECT data acquisitionsystem in this measurement was the same as that in themock-up test. The measured result of the relationshipbetween the probe tilt angle and the output voltage of singlecoil at a frequency of 500 kHz is shown in Figure 12. The tiltdirection is 0° at constant direction. The output voltagemonotonically increased by the increase of tilt angle. Weassumed that the output voltage is proportional to the tiltangle and used the function of linear approximation as anevaluation formula to estimate the tilt angle from theoutput voltage in the mock-up test.

5.2 Estimation of probe tilt angle under scanning inmock-up test

The output voltage of single coil was measured whilemoving the ECT probe on the J-welds of the BMI mock-upat a frequency of 500 kHz. The probe tilt angle underscanning from the measured output voltage could beroughly estimated using the evaluation formula asdescribed previously. The estimated probe tilt angle isshown in Figure 13. The average and the maximum angleswere 2.6° and 8.5°, respectively. As the photographs show in

Fig. 12. Relationship between probe tilt angle and outputvoltage of single coil.

Figure 13, the probe came into contact with the surfaces ofJ-welds on most of the scanning range. Our goal for theprobe tilt angle is within 3° on all the scanning rangebecause it was previously confirmed that the sensitivity ofthis developed ECT probe for themachined slit of 0.5 mm indepth and 0.4 mm in width decreased nearly 1 dB when theprobe tilt angle increased from 0° to 3° [15]. It wasconsidered that the cause of tilt angle of more than 3° on thepartial scanning range is the accuracy of installationposition between the multi-axis robot and the BMI mock-up. The highly accurate measurement and the correction ofinstallation position are the action assignments for theinspection of actual plant.

6 Conclusions

The ECT for the whole weld area on the BMI mock-up wasdemonstrated using the developed ECT system andprocedure in order to verify the defect detection capabilityfor the BMI welds. The surface shape of weld area on theBMI mock-up was measured for generating the scanningtrajectory of ECT probe. The space coordinates and thenormal vectors at the scanning points as the scanningtrajectory were calculated based on the measured results ofweld surface shape. Each motion-axis position of the multi-axis robot corresponding to each scanning point wascalculated by the inverse kinematic algorithm. The BMImock-up test was performed using the developed ECTprobe with the cross coil in the differential mode. The

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artificial SCC and EDM slits given on the build-up weldarea were detected in the mock-up test. From the result ofdetecting defects, it is shown that this ECT system candetect a defect of approximately 2.3 mm in length, 0.5 mmin depth and 0.2 mm in width as the defect detectioncapability for the BMI welds. It was estimated that theaverage and the maximum probe tilt angles were 2.6° and8.5°, respectively. The highly accurate measurement andthe correction of installation position between the multi-axis robot and the inspected BMI for controlling the probetilt angle are the action assignments for the actual use.

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Cite this article as: Noriyasu Kobayashi, Souichi Ueno, Naotaka Suganuma, Tatsuya Oodake, Takeshi Maehara, Takashi Kasuya,Hiroya Ichikawa, Eddy current testing system for bottom mounted instrumentation welds, EPJ Nuclear Sci. Technol. 1, 4 (2015)