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The nonlinear scattered waves increase with increasing wave steepness and a second pulse is evident in the higher-order scattered wave fields.
Based on the computed results, the conditions under which scattered wave modes would significantly increase the intensity of transmitted waves are identified.
Starting from classical absorbing boundary conditions, we propose a method for the separation of time-dependent scattered wave fields due to multiple sources or obstacles.
Both the mean and the scattered wave fields exist in the same perfectly stratified earth medium, without the presence of the irregular interface.
Several numerical tests were conducted to ensure stable solution convergence; the scattered wave fields generated by using the developed method for some case studies were compared with those of finite element analysis.
Numerical examples for 1 MHz and 2.25 MHz transducers are given and scattered wave fields generated by holes of different diameters in an aluminum half-space are compared with the wave fields generated in the defect-free environment.
Specifically, the BIEM is used for computing stress intensity factors and scattered wave displacement amplitudes for an inclined line crack in an otherwise inhomogeneous continuum that is being swept by either pressure waves or vertically polarized shear waves at an arbitrary angle of incidence with respect to the horizontal direction.
The resonant situation is considered when the frequencies of incident (scattered) wave ω1 ω2) are close to E0 + Δ0, i.e., resonance with the spin-orbit split-off band takes place (E0 and Δ0 are the band parameters of the bulk AIIIBV semiconductor).
Both, the back scattered wave and the wave created by absorption directly in the object were detected by the piezoelectric ring sensor described above, which was mounted coaxially to the acoustic axicon.
For instance, a relevant information is the relation between the fractal dimension of the scattering surface and the scattered wave.
The scatterers are located within a region of size D around x A and x B. The far-field scattered wave from the scatterers is theoretically calculated by using a first-order Born approximation.
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CEO of Professional Science Editing for Scientists @ prosciediting.com