Electromagnetic Testing Chapter 3- Electromagnetic Testing

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Materials with high permeability or conductivity have relatively shallow skin depths. At 5kHz, the following materials exhibit the approximate skin depths shown. • Mild steel ~0.1mm • Aluminum, tungsten, zinc ~1 to 2mm • Titanium, stainless steel, and Inconel ~5 to 8mm When there are no defects, uniform current flows in the Y-direction and the magnetic field is uniform in the X- irection perpendicular to current flow and other magnetic components are zero. Charlie Chong/ Fion Zhang
3.19.2 Bx and Bz Components The presence of a defect diverts current away from the deepest part of the crack and concentrates it near the ends of the crack. This produces strong peaks and troughs in B z above the ends of the crack, while B x shows a broad dip along the entire defect length with its amplitude related to depth. Since current lines are close together at the ends of the crack, there are also positive B x peaks at each end of the B x trough. With a forward probe scan, Bz values decrease steadily from background level to the first trough half and subsequently increase to the maximum point near the end of the trough. Figure 3.46 shows typical plots of B x and B z . B z starts at a trough and ends at a peak or the value of B z starts at a peak and ends at a trough depending on the direction of current flow. The curve of B z is insensitive to the speed and lift-off of the probe, and the length of the crack. B z is used to determine if there are cracks in the surface of the part or weld, and calculate their length. 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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For maximum sensitivity, the Circog
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3.14 MAGNETIC FLUX LEAKAGE TESTING
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Page 179 and 180: 3.17.1 Introduction In 1911, Dr. He
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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
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Page 203 and 204: 3.18.1 EMATs Advantages Over Piezoe
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Page 209 and 210: 3.19 ALTERNATING CURRENT FIELD MEAS
Page 211 and 212: 3.19.1 Acfm Principles Of Operation
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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
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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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Electromagnetic Testing Chapter 3- Electromagnetic Testing

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