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Mode conversion

For defect sizing by TOED, use of L waves involves a penalty in resolution of almost a factor of two at a given frequency because of difference in velocity as compared to shear waves and use of SV waves runs into difficulties because of the mode conversion problems. Further, problems due to couplant thickness variations, surface roughness affects, beam skewing and distortion problems in anisotropic welds can also be expected. On the contrary, SH waves are not affected... [Pg.721]

The transmission coefficient Cl (Qj,t), considering transient (broadband) sources, is time-dependent and therefore accounts for the possible pulse deformation in the refraction process. It also takes account of the quantity actually computed in the solid (displacement, velocity potential,...) and the possible mode-conversion into shear waves and is given by... [Pg.736]

The beam-defect interaction is modelled using Kirchhoff s diffraction theory applied to elastodynamics. This theory (see [10] for the scattering by cracks and [11] for the scattering by volumetric flaws) gives the amplitude of the scattered wave in the fonn of coefficients after interaction with defects and takes account of the possible mode-conversion that may occur. [Pg.738]

In UltraSIM/UlSim the ultrasonic sound propagation from a virtual ultrasonic transducer can be simulated in ray tracing mode in any isotropic and homogeneous 3D geometry, including possible mode conversions phenomenons, etc. The CAD geometry for the simulation is a 3D NURBS surface model of the test object. It can be created in ROBCAD or imported from another 3D CAD system. [Pg.871]

Mobility control, issues in, 18 626 Mobility control agents polyacrylamides as, 18 625 in polymer flooding, 18 622 Mobility control surfactants, in enhanced oil recovery, 18 625-628 Mobilizable vectors, for genetic manipulation, 12 471 Mobilization, of ascorbic acid, 25 771 Modacryhc fibers, 9 192 11 188, 189, 190 dyesite content of, 11 195 flame resistance of, 11 214 flammability of, 11 194 pigmented, 11 213 U.S. production of, 11 220t Mode conversion phenomenon, 17 422 Model agreements, 24 373-374 Model-based methods, for reliability, 26 1044... [Pg.593]

Th. D. Happ, M. Kamp, and A. Forchel, Photonic crystal tapers for ultracompact mode conversion. Optics Letters 26, 1102-1104 (2001). [Pg.280]

Fig. 4.4. Reflections from various interfaces in an acoustic microscope, (a) Paths travelled by the rays the broken line shows a ray that returns as a shear wave after mode conversion from a longitudinal wave (or vice versa), (b) The arrival time and magnitude of each reflected ray in (a) the broken lines show the earlier arrival times of reflections from the specimen surface when the specimen is defocused towards the... Fig. 4.4. Reflections from various interfaces in an acoustic microscope, (a) Paths travelled by the rays the broken line shows a ray that returns as a shear wave after mode conversion from a longitudinal wave (or vice versa), (b) The arrival time and magnitude of each reflected ray in (a) the broken lines show the earlier arrival times of reflections from the specimen surface when the specimen is defocused towards the...
Dithiocarbamate -insecticides - Hall electrolytic conductivity in S mode Conversion of -insecticide to carbon disulphide [675]... [Pg.343]

In the next section, we will also address nonconventional storage modes (conversion reaction, interfacial storage), which can provide significant energy densities. Yet it remains to be seen whether or not they can be made reversible enough as to compete with single- and two-phase storage. [Pg.236]

In batch mode, conversions of up to 92.5% were achieved under the above mentioned conditions (Table 6.5). More complete conversions for a continuous reactor design would require intermittent removal of excess methanol and water, possible by flashing the wet methanol. To simulate a continuous process with removal of water a batch experiment was subjected to three repeat cycles of flashing water and methanol, resulting in an acid value 0.5 mg KOH/g for the crude ester product. [Pg.123]

For a viscoelastic material both K and G are complex quantities. When the material sample has finite dimensions other modes of wave propagation may occur as a result of multiple scattering from the material boundaries. Mode conversion from longitudinal wave to shear wave, and vice versa, occurs on reflection at a solid boundary. For material samples in the form of thin rods or plates the modes of wave propagation are extenional waves (with speed determined by the Young s modulus, or the plate modulus), and flexural (bending) waves [8]. [Pg.181]

A second mechnism for sound attenuation is mode conversion. The sound waves in air or water are longitudinal waves, where the particle motion is parallel to the direction of sound propagation. With appropriate boundary conditions the longitudinal deformation can be converted to shear deformation or to viscous flow. Conversion to viscous flow is most readily achieved at... [Pg.182]

Opp is the longitudinal to longitudinal or p to p-wave" scattering cross section of an isolated scatterer. At low frequencies it is primarily associated with the monopole scattering mode. Ops is the mode conversion or longitudinal to shear wave or p to s-wave cross section. It is primarily associated with the dipole mode at low frequencies, oa is the absorption cross section which describes energy dissipation inside viscoelastic inclusions (embedded in an otherwise elastic matrix material). It is active in all modes of excitation. Combining Equation 29 and 30 yields... [Pg.236]

In rigid matrix materials, which support shear waves because of their shear rigidity, mode conversion scattering by heavy solid inclusions predominates at low frequencies (ops opp). In that case a reduces to... [Pg.237]

Soft matrix materials do not support shear waves and consequently dipole scattering by solid inclusions and mode conversion effects are weak in such materials. The corresponding resonance frequency is given by Equation (19), Mode conversion is also weak in the case of cavities in soft materials. The dipole resonance frequency is given by Equation (28), In the case of cavities in soft materials, monopole scattering predominates at low frequencies. The lowest resonance frequency is given by Equation (18) and a reduces to... [Pg.238]

In a rigid matrix material, the low frequency resonance structure of cavities tend to be smeared out and overlapping. Monopole scattering is then relatively weak, but dipole and quadrupole scattering, with accompanying mode conversion, enhance attenuation throughout the low frequency region. [Pg.238]

Figure 1, The Contribution of Mode Conversion Scattering to Longitudinal Stress Wave Attenuation by Spherical Pb Inclusions in Epoxy (Attenuation = 20a log 10(e) = 8.69a)... Figure 1, The Contribution of Mode Conversion Scattering to Longitudinal Stress Wave Attenuation by Spherical Pb Inclusions in Epoxy (Attenuation = 20a log 10(e) = 8.69a)...
Acoustic-absorbing material measurement of acoustic properties, 248 selection for underwater application, 248 Acoustic attenuation mechanisms mode conversion, 182-187 redirection of sound, 182 scattering of sound, 185-194... [Pg.456]

We have shown now that the PTR is a device with excellent polarization purity over a broad frequency range and a low mode conversion loss. The measured performance of a PTR in the near-millimeter band when used... [Pg.305]


See other pages where Mode conversion is mentioned: [Pg.221]    [Pg.221]    [Pg.737]    [Pg.738]    [Pg.902]    [Pg.184]    [Pg.469]    [Pg.63]    [Pg.8]    [Pg.37]    [Pg.226]    [Pg.57]    [Pg.59]    [Pg.465]    [Pg.4]    [Pg.167]    [Pg.168]    [Pg.183]    [Pg.185]    [Pg.188]    [Pg.238]    [Pg.238]    [Pg.240]    [Pg.246]    [Pg.333]    [Pg.283]    [Pg.155]    [Pg.54]   
See also in sourсe #XX -- [ Pg.182 , Pg.187 ]




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