Electromagnetic Testing Chapter 3- Electromagnetic Testing

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Windowsbased software and laptop computers are used to process the data and determine the location and extent of the flaws. All data can be recorded for later display and analysis. For undersea operations, an unskilled operator can scan structural members while a more experienced topside operator views results, analyzes data, and relays information back to the undersea operator. The method also lends itself to the inspection of heavy machinery and equipment, bridges, heavy rail equipment, and process pipes and vessels. In each case, the extent of the structural problem determines the corrective action that must be taken to extend useful service life. Applications for this method have been increasing exponentially since the 1990s. Charlie Chong/ Fion Zhang
3.19.1 Acfm Principles Of Operation The alternating current field measurement (ACFM) is an electromagnetic technique used for the detection and sizing of surface breaking cracks in metallic components and welds. ACFM combines the advantages of the alternating current potential drop (ACPD) technique, which can size defects without calibration, with the ability of eddy current techniques to work without electrical contact. This is accomplished by inducing a uniform field in the test object. The technique requires a moderate to high level of training in its exploitation. Figure 3.45 shows a half-cycle representation of the technique. Alternating current follows the “skin” or outer surface of a conductor. Charlie Chong/ Fion Zhang
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Electromagnetic Testing Chapter 3-
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Submarine Applications Charlie Chon
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Fion Zhang at Shanghai 6th April 20
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IVONA TTS Capable. Charlie Chong/ F
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Chapter 3. ELECTROMAGNETIC TESTING
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Barkhausen effect The Barkhausen ef
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Barkhausen Noise Charlie Chong/ Fio
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Figure 3.1 Eddy current principle.
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Figure 3.2 Schematic diagram of bas
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Figure 3.3 The effect of conductivi
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Figure 3.3 The effect of conductivi
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Another important influence on coil
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If the conductivity of the material
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Figure 3.5 The effect of a crack on
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FIGURE 8-49 Conductivity curve: (a)
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So far, we have described how eddy
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Figure 3.6 The effects of (a) condu
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3.1.2 Limiting Frequency f g of Enc
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Figure 3.7 The effect of degree of
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Charlie Chong/ Fion Zhang
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Eddy Current Heating Charlie Chong/
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Eddy Current Heating Charlie Chong/
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Eddy currents weaken the original m
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3.2 MAGNETIC FLUX LEAKAGE THEORY Wh
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3D Magnetic Field Charlie Chong/ Fi
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3D Magnetic Field Fig.1 THE PRINCIP
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Based on what we have learned about
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Charlie Chong/ Fion Zhang Figure 3.
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Magnetic Field - Simple Semi Ellipt
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Flux leakage sensors have small dia
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The frequency of the alternating fi
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Figure 3.14 Rotating magnet arrange
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3.3 EDDY CURRENT SENSING PROBES For
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As the probe moves over the defect,
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Figure 3.17 Differential surface co
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Figure 3.19 shows an encircling coi
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The application of eddy current sen
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Baffles and tube sheets. Charlie Ch
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Another important consideration for
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3.4.1 Induction Coils For an induct
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If the diameter of a surface coil i
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3.4.2 Hall Effect Sensors Hall effe
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Figure 3.21 illustrates the Hall ef
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Hall voltage Charlie Chong/ Fion Zh
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Since a 1 gauss (G) field produces
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Figure 3.22 Effect of magnetic fiel
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3.5 FACTORS AFFECTING FLUX LEAKAGE
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Defect & Flux Distribution Charlie
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The distance between adjacent defec
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3.6 SIGNAL-TO-NOISE RATIO The signa
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With flux leakage testing, signal-t
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As shown in Eq. (3.6), test frequen
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The characteristic frequency for a
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Charlie Chong/ Fion Zhang
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Figure 3.23 Magnetization or magnet
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By taking the product of B and H fo
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The rate of change of the opposing
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Figure 3.25 Encircling coils establ
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Figure 3.27 DC-MFL sensor illustrat
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Fill factors apply only to encircli
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For best results with encircling co
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3.11 INSTRUMENT DESIGN CONSIDERATIO
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Charlie Chong/ Fion Zhang Figure 3.
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TABLE 3.2. Comparison of Instrument
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Some general categories of equipmen
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Figure 3.29 UniWest-454 EddyView mu
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Scanner operation uses a separate c
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Figure 3.30 E-Lab model US-450 full
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3.12.3 ETC-2000 Scanner Because of
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ETC-2000 scanner features include:
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3.13 INSTITUT DR. FOERSTER Institut
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It is possible to provide 100% eddy
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Figure 3.33 ET testing of hot coppe
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Page 161 and 162: 3.14 MAGNETIC FLUX LEAKAGE TESTING
Page 163 and 164: ASTM E 570 describes magnetic flux
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Page 167 and 168: Applications involving physical par
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Page 171 and 172: 4. Measure the length of nonwelded
Page 173 and 174: Some general applications for the f
Page 175 and 176: Permanent magnets are the preferred
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Page 179 and 180: 3.17.1 Introduction In 1911, Dr. He
Page 181 and 182: 3.17.2 Early Applications Stresses
Page 183 and 184: Typical roll failures are caused by
Page 185 and 186: This technique has been found to be
Page 187 and 188: Figure 3.38 A comparison of Barkhau
Page 189 and 190: Figure 3.39 Three-channel Rollscan
Page 191 and 192: The appropriate depth of measuremen
Page 193 and 194: 3.17.5 Calibration and Testing Bark
Page 195 and 196: Comparative studies by Kirsti Titto
Page 197 and 198: 3.17.6 Current Applications Barkhau
Page 199 and 200: 3.17.9 Pipe/Tubing/Sheet/Plate Manu
Page 201 and 202: EMATs overcome many common ultrason
Page 203 and 204: 3.18.1 EMATs Advantages Over Piezoe
Page 205 and 206: 3.18.3 Recent Applications And Deve
Page 207 and 208: Figure 3.44 Courtesy of Weld Inspec
Page 209: 3.19 ALTERNATING CURRENT FIELD MEAS
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Page 215 and 216: 3.19.2 Bx and Bz Components The pre
Page 217 and 218: 3.19.3 Butterfly Plot To aid interp
Page 219 and 220: 3.19.4 Probe Design Standard ACFM p
Page 221 and 222: Figure 3.48 Flowchart selection of
Page 223 and 224: 3.31 APPLICATIONS One active encode
Page 225 and 226: Other applications include: • Ins
Page 227 and 228: Eddy Current Testing at High Temper
Page 229 and 230: Good Luck Charlie Chong/ Fion Zhang
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