Electromagnetic Testing Chapter 3- Electromagnetic Testing

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Maximum testing speeds for Rotomat/Transomat systems depend on sensor design and tubing size. Rotomat Ro sensor systems have four rotating heads covering tubing diameters from 20 to 520 mm (0.79 to 20.5 in.).Transomat TR sensor systems have three sensor systems covering tubing diameters from 26 to 440 mm (1.02 to 17.3 in.). The Rotomat Ro 180 sensor system has a limited design range and can scan tubes with diameters ranging from 20 to 180mm (0.79 to 7.09 in.) with throughput speeds of 2.6 m/s (8.5 f/s).The Transomat TR 180 sensor system can also scan tubes with diameters ranging from 26 to 180mm (1.02 to 7.09in.) with throughput speeds of 2.6 m/s (8.5 f/s). The maximum throughput speed for larger diameter tubing and larger Ro and TR sensing heads is about 2 m/s (6.6 f/s), depending on tube diameter. Large, fully automated testing lines, incorporating multiple test parameters, are extensively used in Europe for the inspection of critical piping systems. A schematic representation of a fully integrated material handling and transport system with automatic testing lines is shown in Figure 3.36. Charlie Chong/ Fion Zhang
Charlie Chong/ Fion Zhang Figure 3.36 Schematic representation of complex multifunction test system that combines eddy current, flux leakage, and dimensional testing. Courtesy of Institut Dr. Foerster.
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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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Page 115 and 116: As shown in Eq. (3.6), test frequen
Page 117 and 118: The characteristic frequency for a
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Page 121 and 122: Figure 3.23 Magnetization or magnet
Page 123 and 124: By taking the product of B and H fo
Page 125 and 126: The rate of change of the opposing
Page 127 and 128: Figure 3.25 Encircling coils establ
Page 129 and 130: Figure 3.27 DC-MFL sensor illustrat
Page 131 and 132: Fill factors apply only to encircli
Page 133 and 134: For best results with encircling co
Page 135 and 136: 3.11 INSTRUMENT DESIGN CONSIDERATIO
Page 137 and 138: Charlie Chong/ Fion Zhang Figure 3.
Page 139 and 140: TABLE 3.2. Comparison of Instrument
Page 141 and 142: Some general categories of equipmen
Page 143 and 144: Figure 3.29 UniWest-454 EddyView mu
Page 145 and 146: Scanner operation uses a separate c
Page 147 and 148: Figure 3.30 E-Lab model US-450 full
Page 149 and 150: 3.12.3 ETC-2000 Scanner Because of
Page 151 and 152: ETC-2000 scanner features include:
Page 153 and 154: 3.13 INSTITUT DR. FOERSTER Institut
Page 155 and 156: It is possible to provide 100% eddy
Page 157 and 158: Figure 3.33 ET testing of hot coppe
Page 159 and 160: For maximum sensitivity, the Circog
Page 161 and 162: 3.14 MAGNETIC FLUX LEAKAGE TESTING
Page 163: ASTM E 570 describes magnetic flux
Page 167 and 168: Applications involving physical par
Page 169 and 170: Inexpensive 60 Hz eddy current comp
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
Page 177 and 178: Robot Charlie Chong/ Fion Zhang
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 and 210: 3.19 ALTERNATING CURRENT FIELD MEAS
Page 211 and 212: 3.19.1 Acfm Principles Of Operation
Page 213 and 214: Figure 3.45 Current flow and induce
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3.19.2 Bx and Bz Components The pre
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3.19.3 Butterfly Plot To aid interp
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3.19.4 Probe Design Standard ACFM p
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Figure 3.48 Flowchart selection of
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3.31 APPLICATIONS One active encode
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Other applications include: • Ins
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Eddy Current Testing at High Temper
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Good Luck Charlie Chong/ Fion Zhang
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