Developments in Electromagnetic Inspection Methods II

Similar documents
Multivariate Regression Algorithm for ID Pit Sizing

Electromagnetic Eddy Current Sensors for Evaluation of Sea-Cure and 2205 Duplex Condenser Tubing

ADVANCED COMBINATION PROBE FOR TESTING FERRITIC SEA-CURE CONDENSER TUBING

2.5D Finite Element Simulation Eddy Current Heat Exchanger Tube Inspection using FEMM

Steam Generator Tubing Inspection

FLAW DETECTION USING ENCIRCLING COIL EDDY CURRENT SYSTEMS

Developments in Electromagnetic Inspection Methods I

Acoustic Emission Linear Location Cluster Analysis on Seam Welded Hot Reheat Piping

Detection of Internal OR External Pits from Inside OR Outside a tube with New Technology (EMIT)

Heat Exchanger & Boiler Tube Inspection Techniques

AUTOMATED EDDY CURRENT DETECTION OF FLAWS IN SHOT-PEENED

Simulation Model for SG Eddy Current SG Inspection

INFLUENCE OF SIGNAL-TO-NOISE RATIO ON EDDY CURRENT SIGNALS OF CRACKS IN STEAM GENERATOR TUBES

MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS

Eddy Current Signal Analysis Techniques for Assessing Degradation of Support Plate Structures in Nuclear Steam Generators

Studying the Sensitivity of Remote-Field Testing Signals when Faced with Pulling Speed Variations

Ensuring Shielding adequacy in Lead shielded spent fuel transportation casks using gamma scanning

Magnetic induction with Cobra3

BALANCE FIELD ELECTROMAGNETIC TECHNIQUE INSPECTION REPORT OF THE 8_INCH_1260_FITTING (HA-2/1200 BLOCK) TESTEX, INC. TESTED: JANUARY 9, 2019

Feasibility of Detection of Leaking Fuel Rods Using Side Coupled Guided Waves

Modelling III ABSTRACT

IMPROVEMENT OF DETECTION OF SMALL DEFECTS LOCATED NEAR OR FAR FROM WELDS OF MAGNETIC STEAM GENERATOR TUBES USING REMOTE FIELD EDDY CURRENT

Department of Mechanical and Aerospace Engineering. MAE334 - Introduction to Instrumentation and Computers. Final Examination.

Developments in Ultrasonic Guided Wave Inspection

Instruction Manual Veritest

Proportional-Integral Controller Performance

Magnetic induction with Cobra3

New Multi-Technology In-Line Inspection Tool For The Quantitative Wall Thickness Measurement Of Gas Pipelines

ULTRASONIC SIGNAL CHARACTERIZATIONS OF FLAT-BOTTOM HOLES IN

VALVE CONDITION MONITORING BY USING ACOUSTIC EMISSION TECHNIQUE MOHD KHAIRUL NAJMIE BIN MOHD NOR BACHELOR OF ENGINEERING UNIVERSITI MALAYSIA PAHANG

18th World Conference on Non-destructive Testing, April 2012, Durban, South Africa

EPRI NDE Program Technology Transfer Thinking Ahead...

DEEP PENETRATING EDDY CURRENT for DETECTING VOIDS in COPPER

Magnetics Design. Specification, Performance and Economics

Steady State Operating Curve Voltage Control System

DATA ANALYSIS ALGORITHMS FOR FLAW SIZING BASED ON EDDY CURRENT ROTATING PROBE EXAMINATION OF STEAM GENERATOR TUBES

Module 4 Design for Assembly IIT BOMBAY

MultiScan MS Tube Inspection System. Multi-technology System Eddy Current Magnetic Flux Leakage Remote Field IRIS Ultrasound

Gentec-EO USA. T-RAD-USB Users Manual. T-Rad-USB Operating Instructions /15/2010 Page 1 of 24

MultiScan MS Tube Inspection System. Multi-technology System Eddy Current Magnetic Flux Leakage Remote Field IRIS Ultrasound

R&D of Multi-Frequency ECT Algorithms for FBR SG Tubes

DETECTION OF SUB LAYER FATIGUE CRACKS UNDER AIRFRAME RIVETS

Multiple Frequency Eddy Current Technique

Evaluation of 3C sensor coupling using ambient noise measurements Summary

Enhancement of the POD of Flaws in the Bulk of Highly Attenuating Structural Materials by Using SAFT Processed Ultrasonic Inspection Data

FATIGUE CRACK CHARACTERIZATION IN CONDUCTING SHEETS BY NON

Optimized Semi-Flexible Matrix Array Probes for Large Rotor Shafts and DGS Sizing Diagram Simulation Tool

DEEP FLAW DETECTION WITH GIANT MAGNETORESISTIVE (GMR) BASED SELF-NULLING PROBE

CHAPTER-4 FRUIT QUALITY GRADATION USING SHAPE, SIZE AND DEFECT ATTRIBUTES

Model Correlation of Dynamic Non-linear Bearing Behavior in a Generator

EDDY CURRENT INSPECTION MODELLING OF THE ELBOW OF A STEAM GENERATOR TUBE WITH THE FINITE ELEMENT SOFTWARE «FLUX»

INVESTIGATION OF IMPACT DAMAGE OF CARBON FIBER- RAINFORCED PLASTIC (CFRP) BY EDDY CURRENT NON- DESTRUCTIVE TESTING

Homework Assignment (20 points): MORPHOMETRICS (Bivariate and Multivariate Analyses)

DAMAGE DETECTION IN PLATE STRUCTURES USING SPARSE ULTRASONIC TRANSDUCER ARRAYS AND ACOUSTIC WAVEFIELD IMAGING

Appendix 3 - Using A Spreadsheet for Data Analysis

Corrosion Steel Inspection under Steel Plate Using Pulsed Eddy Current Testing

The shunt capacitor is the critical element

Depth of Penetration Effects in Eddy Current Testing

DIAGNOSTIC OF CORROSION DEFECTS IN STEAM GENERATOR TUBES USING ADVANCED SIGNAL PROCESSING FROM EDDY CURRENT TESTING

COMPUTER MODELING OF EDDY CURRENT TRANSMIT-RECEIVE PROBES FOR. S.P. Sullivan, V.S. Cecco, L.S. Obrutsky, D. Humphrey, S.P. Smith and K.A.

Ultrasonic Detection of Inclusion Type Defect in a Composite Panel Using Shannon Entropy

Chapter 5. Signal Analysis. 5.1 Denoising fiber optic sensor signal

High Resolution Eddy Current Testing of Superconducting Wires using GMR-Sensors

USE OF BASIC ELECTRONIC MEASURING INSTRUMENTS Part II, & ANALYSIS OF MEASUREMENT ERROR 1

RLC-circuits with Cobra4 Xpert-Link

Homework Set 3.5 Sensitive optoelectronic detectors: seeing single photons

PASS Sample Size Software

EDDY CURRENT TECHNOLOGY FOR HEAT EXCHANGER AND STEAM GENERATOR TUBE INSPECTION

A Review on Optimization of Process Parameters for Material Removal Rate and Surface Roughness for SS 202 Material During Face Milling Operation

EDDY CURRENT TESTING

3D Non-Linear FEA to Determine Burst and Collapse Capacity of Eccentrically Worn Casing

QUANTITATIVE COMPUTERIZED LAMINOGRAPHY. Suzanne Fox Buchele and Hunter Ellinger

Non-destructive testing Equipment for eddy current examination Array probe characteristics and verification

Pipeline Inspection Technologies Demonstration Report Final

Influence of Scanning Velocity and Gap Distance on Magnetic Flux Leakage Measurement

Fasteners. Massachusetts Institute of Technology Kavli Institute for Astrophysics and Space Research (MKI) Dwg. No Revision D March 24, 2015

A Numerical Study of Depth of Penetration of Eddy Currents

Department of Mechanical and Aerospace Engineering. MAE334 - Introduction to Instrumentation and Computers. Final Examination.

D DAVID PUBLISHING. Eddy Current Test for Detection of Foreign Material using Rotating Probe. 2. Theory. 1. Introduction

Dave Stubbs, Wally Hoppe, and Bob Olding. NDE Systems Division Systems Research Laboratories, Inc. Dayton, Ohio

Attenuation dependent detectability at ultrasonic inspection of copper

Experiment 2: Transients and Oscillations in RLC Circuits

Tolerancing Primer. Marshall R. Scott. University of Arizona. December 17, 2015

Module 1: Introduction to Experimental Techniques Lecture 2: Sources of error. The Lecture Contains: Sources of Error in Measurement

Reference Manual SPECTRUM. Signal Processing for Experimental Chemistry Teaching and Research / University of Maryland

EE351 Laboratory Exercise 4 Field Effect Transistors

In-line eddy current testing of wire rod

Probability of Rejection - In conformance with DNV OS F101

Development of the Electrical and Magnetic Model of Variable Reluctance Speed Sensors

ROHM Stepper Motor Driver Evaluation and Applications

Experiment 9: AC circuits

Flexible PCB-Based Eddy Current Array Probes for the Inspection of Turbine Components

Vertical Shaft Plumbness Using a Laser Alignment System. By Daus Studenberg, Ludeca, Inc.

A Prototype Wire Position Monitoring System

DEVELOPMENT OF A STRUCTURAL SYSTEM RELIABILITY FRAMEWORK FOR OFFSHORE PLATFORMS

Long Range Ultrasonic Testing - Case Studies

CHAPTER 5 Test B Lsn 5-6 to 5-8 TEST REVIEW

Properties of Magnetism

Page 21 GRAPHING OBJECTIVES:

Surveillance and Calibration Verification Using Autoassociative Neural Networks

Transcription:

6th International Conference on NDE in Relation to Structural Integrity for Nuclear and Pressurized Components October 2007, Budapest, Hungary For more papers of this publication click: www.ndt.net/search/docs.php3?mainsource=70 Developments in Electromagnetic Inspection Methods II ID Pit Sizing Utilizing Two Variable Regression Curves N. Muthu, EPRI, USA; C.J. Speas, Anatec International, USA; F. Hall, Wolf Creek Nuclear Operating Corp., USA ABSTRACT The traditional approach to ID pit sizing involves the use of one variable, amplitude or phase angle to depth, measurement curves. Industry experience has shown that these one variable techniques have shortcomings when ID flaws vary in morphology. Phase and amplitude of an eddy current signal are dependent on both the depth and the total volume of ID pits. These two variables can be used to construct a two variable regression curve relating to depth. A two variable curve should attenuate the effect of pit diameter on depth estimates. Calibration data sets consisting of machined pits of various diameters and depths were acquired. Two variable regression curves were used to estimate the depth of machined pits of various diameters and depths. Traditional one variable curves were also used to estimate the depth of these indications. The results of these analyses were evaluated to determine sizing accuracy using a standard regression plot to document performance of the data against the best fit. Based on this analysis it was identified that two variable regression analysis consistently provided more accurate ID pit sizing. CITATIONS AND ACKNOWLEDGEMENTS This paper was prepared utilizing materials provided by: NLREG Regression Analysis Software Kenji Krzywosz, EPRI NDE Center Nathan Muthu, EPRI NDE Center Duke Energy Materials Engineering & Lab Services ID Pit sizing for Admiralty Brass Tubing presented at the Fifth EPRI BOP Heat Exchanger NDE Symposium, Kevin Newell and Kenji Krzywosz EPRI Electromagnetic NDE Guide for Balance-of-Plant Heat Exchangers, Rev.2 The authors also acknowledge and thank: The Wolf Creek QC/NDE group for their tireless effort in the implementation of the BOP NDE Program. This study would not have been possible without their dedication and expertise. Andrew Neff, Anatec International, for his insight and guidance in the preparation of the study. INTRODUCTION AND BACKGROUND This paper documents the results of a study undertaken to determine if ID pit depth sizing (by the ET method) could be improved by utilizing two variable calibration curves. The central thesis of this study was to ascertain if a single measurement curve, constructed using two variables, would provide improved sizing performance on a variety of ID pit morphologies. The study was limited to copper based alloys, 90/10 CuNi and SB-111, Admiralty Brass. The traditional approach to ID pit sizing involves the use of one variable, amplitude or phase angle to depth measurement curves. One variable measurement curves have provided less than optimum results when sizing ID pit depths. The phase and amplitude of an eddy current signal are dependent on the depth as well as the total volume and shape of a flaw. This statement is validated by both eddy current theory and observation. A two variable function relating signal amplitude and phase to depth should help to attenuate the effects of pit volume.

Commercially available calibration curve functions in eddy current software packages do not support the use of two variables. In order to construct the two variable calibration curves regression analysis software was procured from NLREG. The goal of regression analysis is to determine the values of parameters for a function that cause the function to best fit a set of provided data observations. In this study two types of regression analysis techniques were utilized: 1. Linear regression analysis was utilized to evaluate sizing performance of the afore-mentioned ET analysis techniques. 2. Multivariate regression analysis was utilized for the development of the two variable (amplitude and phase) curves. METHODOLOGY AND TEST PERFORMANCE The principal question addressed by this study was: Can a single measurement curve accurately depth size ID pits of various morphologies? This study addresses this question by measuring ID defects ranging in size from.0625 round to.250 X.125 elongated artificial defects; a smaller sample of real world ID defects was also measured. All of these defects were measured using three separate techniques Vpp phase angle analysis, VertMax amplitude analysis, and two-variable analysis (VertMax amplitude and Vpp phase angle). The results of these analyses were then evaluated for sizing accuracy. Study Overview 1. Construct two variable curves and develop a working model for ID pit sizing. 2. Perform depth sizing of available data using both two variable and traditional one variable techniques. 3. Apply adequate rigor to test samples to assure representative pit sizes and morphologies are evaluated. The data employed should contain defects of different morphologies (e.g. round pits, elongated pits) 4. Evaluate depth sizing accuracy of two variable and one variable curves on a variety of pit morphologies. Software The NLREG software requires the development of an initial equation in order to generate the measurement curves. This equation used in this study contained three distinct elements: Independent Variables Phase and Amplitude of Indications Dependent Variable Depth of Indications Estimation Parameters Parameters used during regression analysis to generate the best fit curve The equation was constructed so that the curve generated matched the data values of the control set as closely as possible. The equation was developed using the following steps: Record phase, amplitude, and depth measurements from a control set of calibration standard defects and field samples. This control set contained data from as many ID defects as possible. Experiment using various equations to determine the equation which best fits the control data set as a whole. Examination of the regression output data generated during this process helped to validate the equation. A primary consideration was to validate that the equation and software generated the measurement curve in the same general form whether all available defect data was included or only selected data points were used.

The following tables are regression analysis output screens from the NLREG software depicting results from an initial equation generated early in the study and also the final equation used. An explanation of selected terms used in the analysis is also included. PIT SIZING ALGORITHM Table 1 Early Function Standard error of estimate = 23.5455 Average deviation = 18.7966 Maximum deviation for any observation = 37.3027 Proportion of variance explained (R^2) = 0.6127 (61.27%) Adjusted coefficient of multiple determination (Ra^2) = 0.5804 (58.04%) Table 2 Final Function PIT SIZING ALGORITHM Standard error of estimate = 2.50431 Average deviation = 1.53664 Maximum deviation for any observation = 6.22881 Proportion of variance explained (R^2) = 0.9956 (99.56%) Adjusted coefficient of multiple determination (Ra^2) = 0.9953 (99.53%) Explanation of Analysis Terms Table 3 Average and Maximum Deviation The "Average deviation'' is the average over all observations of the absolute value of the difference between the actual value of the dependent variable and its predicted value. The "Maximum deviation for any observation'' is the maximum difference (ignoring sign) between the actual and predicted value of the dependent variable for any observation. Proportion of Variance Explained The "Proportion of variance explained (R2)'' indicates how much better the function predicts the dependent variable than just using the mean value of the dependent variable. Adjusted Coefficient of Multiple Determination The "adjusted coefficient of multiple determination (Ra2)'' is an R2 statistic adjusted for the number of parameters in the equation and the number of data observations. It is a more conservative estimate of the percent of variance explained, especially when the sample size is small compared to the number of parameters.

The following figures are curves generated from the NLREG software representing one variable and two variable techniques. Figure 1 - One Variable Curve Figure 2 - One Variable Curve

Figure 3 - Three Dimensional Representation Figure 4 - Two Dimensional Representation (Looking Down)

Measurement Methodology Depth measurements of artificial defects of known depths and morphology were performed in order to assess sizing accuracy. The following process was used: Data on phase and amplitude from the standard entries used for setup were recorded and input into the regression analysis software to construct the two- variable, Amplitude & Phase vs. Depth Curves. Traditional one variable curves were constructed in the ET analysis software. The following calibration curves were established: o Prime Frequency (Vvm) Amplitude & (Vpp) Phase vs. Depth- Using a 0, 0, 0 point, various 100% TWHs, and the ~50% defect measurements from the standards. The two variable curve was established using only the 0,0,0 point, the 100% TWH signals and the 50% ID signals to simulate a typical field calibration methodology. (Vpp) Phase vs. Depth Using 1/8 diameter pits o Low Frequency (~F 0 /8) (Vvm) Amplitude vs. Depth Using 1/8 diameter pits The above calibration curves were utilized to analyze the following ET data sets: o.625 X.049 90/10 CuNi tubing containing calibration standard entries with various pit morphologies. Each standard was recorded four times and the standard was rotated ninety degrees between pulls. This practice induced variations to the signal phase and amplitude dependent on how the coil was affected by the ID defect. o EPRI provided data set of.625 X.049 Admiralty Brass tubing containing standard entries with various pit morphologies o Data sets from field samples that had been removed from service and destructively analyzed.

The following table shows a sample of data recorded during the measurement phase of the study. Table 4

The following table and figures detail a portion of the field sample tubes examined. Note the variation in ID pit morphologies present. Table 5 Tube Pit Description Depth (mils) Percent depth 10-31 1 Tight pit cluster, 1/8" diameter 16 32 2 Pit cluster, 1/4" diameter 17 35 3 Arc-shaped pit cluster, 1/4" axial extent 30 61 3A 3/16" diameter pit 25 51 4 3/16" diameter pit 36 73 4A Two joined pits, 1/4" axial extent 27 55 5 Several discrete pit, deepest 1/8" diameter 30 61 6 Several discrete pit, deepest 1/8" diameter 19 39 19-35 1A 1/16" diameter pit 22 45 1B Two 1/16" diameter pits na na 2A 1/16" diameter pit 16 33 2B One 1/16" diameter pit, several smaller pits na na 3 3/32" diameter pit 16 33 Figure 5 - Tube 10-31, pit location #3 Figure 6 - location #3 section view Figure 7 - Tube 10-31, pit location #5 Figure 8 - location #5 section view

Figure 9 - location #3 section view Figure 10 - Tube 19-35, pit location #3 Figure 11 - Tube 10-31, location #6 Figure 12 - location #6 section view SIZING PERFORMANCE RESULTS Defect depth sizing was evaluated using the linear regression analysis technique. This technique was used in the preparation of the EPRI Electromagnetic NDE Guide for Balance-of-Plant Heat Exchangers, and many of the same parameters are utilized in this document. The Excel-based spreadsheet for performing this analysis is available from EPRI. This evaluation technique compares the depth measurements from the various techniques to the physically measured depth of the defects. Three values are generated during the regression analysis that can be used to gauge sizing accuracy: slope of the regression line, correlation coefficient, and root mean square error (RMSE). A fourth value was also included during the evaluation Maximum Deviation. This value reflects the largest variance when depth sizing a specific defect in a data set. Flaw depth sizing results improve as the correlation coefficient increases, the slope of the linear regression line approaches one, and the RMSE and Maximum Deviation values decrease.

Table 6 Value Minimum Criteria Ideal Slope of Regression Line >0.7 &<1.3 1.0 Correlation Coefficient >70% 100% RMSE <20% 0% Maximum Deviation None Established 0% The following table summarizes the average sizing accuracy of the different measurement techniques evaluated. 1 Variable Amplitude Table 7 1 Variable Phase Angle 2 Variable Amplitude & Phase Slope of Regression Line.802.812.852 Correlation Coefficient 74.6 91.9 97.9 RMSE 22.54 11.80 6.49 Maximum Deviation 54.66 23.00 12.66 Regression plots for each technique and each sample set used in calculating average sizing accuracy are shown in Figures 13 through 21. The following three plots reflect sizing accuracy on the EPRI provided Admiralty Brass data set. Figure 13 - Low Frequency Amplitude vs. Depth Technique Note: Maximum deviation, and RMSE

Figure 14 - Prime Frequency Phase vs. Depth Technique Note: Maximum deviation, correlation coefficient and RMS are improved Figure 15 - Prime Frequency Two Variable Technique Note: Low maximum deviation, high correlation and low RMSE

The following three plots reflect sizing accuracy on the Wolf Creek 90/10 Copper Nickel data set. Numerous calibration standards of various morphologies were utilized in this data set. Figure 16 - Low Frequency Amplitude vs. Depth Technique Note: Larger data set. Maximum deviation and RMSE are high Figure 17 - Prime Frequency Phase vs. Depth Technique Note: Maximum deviation, correlation coefficient and RMSE are improved over Figure 16

Figure 18 - Prime Frequency Two Variable Technique Note: Low maximum deviation, high correlation and low RMSE The following three plots reflect sizing accuracy on a data set of actual flaws in 90/10 Copper Nickel tubes removed from service at Wolf Creek. This data set contained the fewest number of defects. Figure 19 - Results from a set of flaws from destructively analyzed tubes

Figure 20 - Results from a set of flaws from destructively analyzed tubes Figure 21 - Results from a set of flaws from destructively analyzed tubes

The following two plots were not used in the overall average calculations. They are shown to illustrate the performance of the two variable technique in specific situations. Figure 22 NOTE - This plot is shown to illustrate the accuracy obtained using only 100% flaws of various morphologies as calibration points Figure 22 NOTE - Results of two variable technique when only round ID flaws are used for calibration and only round ID flaws are depth sized

CONCLUSIONS AND RECOMMENDATIONS Conclusions 1. Amplitude analysis was found to provide the lowest correlation and highest RMS error of the techniques evaluated. 2. Phase angle analysis was found to provide better correlation and lower error (more accurate) than the amplitude analysis. 3. Two variable analysis, using phase angle and amplitude, provided the best correlation factor and lowest RMS error of all techniques evaluated. 4. Pit shape, or morphology, had an adverse effect on pit sizing in all three of the techniques analyzed; two variable analysis tended to attenuate this effect. Recommendations 1. Two variable measurement curves should be considered for integration into commercially available ET analysis software. 2. Continued validation of the two variable measurement technique utilizing field data with destructive analysis is warranted.