UT Testing-Section 2 Physics of Ultrasound

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Q10: For a shear wave travelling from steel to water incident on the boundary at 10 degrees will give a refracted shear wave in water with an angle <strong>of</strong>: A. 0 degrees B. 5 degrees C. 20 degrees D. none <strong>of</strong> the above
Page 1: Section 2: Physics of Ultrasound
Page 4 and 5: 2.0: Ultrasound Formula http://www.
Page 6 and 7: Ultrasonic Formula
Page 9 and 10: 2.1: Wave Propagation Ultrasonic te
Page 11 and 12: Acoustic Spectrum
Page 13 and 14: Acoustic Wave - Node and Anti-Node
Page 15 and 16: http://hyperphysics.phy-astr.gsu.ed
Page 17 and 18: 2.2: Modes of Sound Wave Propagatio
Page 19 and 20: Longitudinal and shear waves
Page 21 and 22: Longitudinal and shear waves
Page 23 and 24: 2.2.3 Longitudinal Wave Also Knows
Page 25 and 26: Longitudinal wave: Longitudinal wav
Page 28 and 29: 2.2.4 Shear waves (S-Waves) In air,
Page 30 and 31: Shear waves
Page 34 and 35: 2.2.5 Rayleigh Characteristics Rayl
Page 36 and 37: Rayleigh waves
Page 38 and 39: Surface (or Rayleigh) waves travel
Page 40 and 41: The major axis of the ellipse is pe
Page 42 and 43: Surface wave or Rayleigh wave are f
Page 44 and 45: Surface wave - Following Contour Su
Page 46 and 47: Rayleigh Wave http://web.ics.purdue
Page 48 and 49: Love Wave
Page 50 and 51: At this depth, wave energy is about
Page 52 and 53: Q: Which of the following modes of
Page 54 and 55: Since the 1990s, the understanding
Page 56 and 57: Plate or Lamb waves are the most co
Page 58 and 59: Plate wave or Lamb wave are formed
Page 60 and 61: When guided in layers they are refe
Page 62 and 63: Symmetrical = extensional mode Asym
Page 64 and 65: Other Reading: Lamb Wave Lamb waves
Page 66 and 67: Fig. 4 Diagram of the basic pattern
Page 68 and 69: 2.2.7 Dispersive Wave: Wave modes s
Page 70 and 71: Plate or Lamb waves are generated a
Page 72 and 73: 2.3: Sound Propagation in Elastic M
Page 74 and 75: Spring model- A mass on a spring ha
Page 76 and 77: Elastic Model
Page 78 and 79: Elastic Model / Longitudinal Wave
Page 80 and 81: Elastic Model / Shear Wave
Page 82 and 83:
Since the mass m and the spring con
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Elastic constant → spring constan
Page 86 and 87:
Q163 Acoustic velocity of materials
Page 88 and 89:
When calculating the velocity of a
Page 90 and 91:
It must also be mentioned that the
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Longitudinal Wave Velocity: V L The
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2.4: Properties of Acoustic Plane W
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http://www.ndt-ed.org/EducationReso
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Java don’t work? Uninstalled →
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Java don’t work? http://jingyan.b
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Java don’t work? http://jingyan.b
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The velocities sound waves The velo
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2.5: Wavelength and Defect Detectio
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Keywords: • Discontinuity must be
Page 110 and 111:
Keywords: • Coarse grains →Lowe
Page 112 and 113:
Coarse grains →Lower frequency to
Page 114 and 115:
Keywords: • Higher the frequency,
Page 116 and 117:
2.5.3 Further Reading Detectability
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Determining cross sectional area us
Page 121 and 122:
“Sonic pulse volume” and S/N (d
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2.6: Attenuation of Sound Waves 2.6
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Absorption: Sound attenuations are
Page 127 and 128:
Anisotropic Columnar Grains with di
Page 129 and 130:
The amplitude change of a decaying
Page 131 and 132:
Attenuation is generally proportion
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Amplitude at distance Z where: Wher
Page 135:
2.6.2 Factors Affecting Attenuation
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2.6.4 Further Reading on Attenuatio
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Q168: Heat conduction, viscous fric
Page 142 and 143:
2.7: Acoustic Impedance Acoustic im
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Sound travels through materials und
Page 146 and 147:
Reflection/Transmission Energy as a
Page 148 and 149:
Q2.8: The acoustic impedance of mat
Page 150 and 151:
When the acoustic impedances of the
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Reflection Coefficient:
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Using the above applet, note that t
Page 156 and 157:
Incident Wave other than Normal? -
Page 158 and 159:
Q: The figure above shown the parti
Page 160 and 161:
For example: The dB loss on transmi
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Q6: For an ultrasonic beam with nor
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Refraction and Snell's Law When an
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Refraction takes place at an interf
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Snell's Law describes the relations
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Snell Law http://www.ndt-ed.org/Edu
Page 175 and 176:
When a longitudinal wave moves from
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Refraction and mode conversion occu
Page 179 and 180:
For example, calculate the first cr
Page 181 and 182:
Snell Law: 1 st / 2 nd Critical Ang
Page 183 and 184:
Q. Both longitudinal and shear wave
Page 191 and 192:
Typical angle beam assemblies make
Page 193 and 194:
Depth & Skip
Page 195 and 196:
Second Critical Angle The second cr
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2.10: Mode Conversion When sound tr
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In the previous section, it was poi
Page 201 and 202:
Snell's Law
Page 203 and 204:
Reflections
Page 205 and 206:
V S1 V S2
Page 207 and 208:
Snell Law- 1 st & 2 nd Critical Ang
Page 209 and 210:
Transverse wave can be introduced i
Page 211 and 212:
Calculate the offset for following
Page 213 and 214:
Refraction and mode conversion at n
Page 215 and 216:
Refraction and mode conversion at n
Page 217 and 218:
Q1. From the above figures, if the
Page 219 and 220:
Q: On Calculation: Incident angle=
Page 221 and 222:
Q1. If you were requested to design
Page 223 and 224:
2.11: Signal-to-Noise Ratio In a pr
Page 225 and 226:
The following formula relates some
Page 227 and 228:
Rather than go into the details of
Page 230 and 231:
Determining cross sectional area us
Page 232 and 233:
“Sonic pulse volume” and S/N (d
Page 234 and 235:
Pulse Length
Page 236 and 237:
2.12: The Sound Fields 2.12.1 Wave
Page 238 and 239:
When waves interact, they superimpo
Page 240 and 241:
UT Transducer http://www.fhwa.dot.g
Page 242 and 243:
UT Transducer
Page 244 and 245:
Wave Interaction Complete in-phase
Page 246 and 247:
With an ultrasonic transducer, the
Page 248 and 249:
29. It is possible for a discontinu
Page 250 and 251:
2.12.2 Variations in sound intensit
Page 252 and 253:
The sound wave exit from a transduc
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The Near Field (Fresnel) and the Fa
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Amplitude ← Near Field Effect: Be
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Near field (near zone) or Fresnel z
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Near/ Far Fields http://miac.unibas
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where α is the radius of the trans
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The curvature and the area over whi
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Fresnel & Fraunhofer Zone
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Fresnel & Fraunhofer Zone http://st
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Q4: A transducer has a near field i
Page 272 and 273:
2.12.4 Dead Zone In ultrasonic test
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Dead Zone -The initial pulse is a t
Page 276 and 277:
Dead Zone Illustration http://www.n
Page 278 and 279:
Q: On an A-scan display, the “dea
Page 280 and 281:
2.13: Inverse Square Rule/ Inverse
Page 282 and 283:
Small Reflector, a reflector smalle
Page 286 and 287:
2.14: Resonance Another form wave i
Page 288 and 289:
Thickness of Crystal at Fundamental
Page 290 and 291:
Resonance UT Testing- The diagram b
Page 292 and 293:
From the natural frequencies it is
Page 294 and 295:
Q: The formula used to determine th
Page 296 and 297:
2.15 Measurement of Sound
Page 298 and 299:
Ultrasonic Formula - Signal Amplitu
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where: delta X is the difference in
Page 302 and 303:
From this table it can be seen that
Page 304 and 305:
However, the power or intensity of
Page 306 and 307:
Revising the table to reflect the r
Page 308 and 309:
Sound Levels- Relative dB
Page 310 and 311:
“Absolute" Sound Levels Sound pre
Page 313 and 314:
dB meter 97.3dB against standards s
Page 315 and 316:
Exercise: Find the absolute sound l
Page 317 and 318:
Practice: dB
Page 319 and 320:
Example Calculation 2 If the intens
Page 321 and 322:
What is the absolute rock concert s
Page 323 and 324:
Practice Makes Perfect 28. An advan
Page 325 and 326:
学习总是开心事
Page 327 and 328:
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UT Testing-Section 2 Physics of Ultrasound

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