2017
DOI: 10.1016/j.apacoust.2016.11.019
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Modeling of random ground roughness effects by an effective impedance and application to time-domain methods

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Cited by 4 publications
(2 citation statements)
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“…Thus, the first ground dip is located at a frequency of 500 Hz for the unperturbed problem, but in the random case it is at 495 Hz for L ¼ 0.5 m and 490 Hz for L ¼ 5 m. This effect was also noticed for random roughness. 22 Besides, the agreement between the mean pressure computed with the Bourret approximation and by an ensemble-averaging over 200 realizations is satisfactory. In particular, for L ¼ 0.5 m, the curves depicting these two solutions are almost superimposed for both receiver heights.…”
Section: A Numerical Specificationmentioning
confidence: 70%
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“…Thus, the first ground dip is located at a frequency of 500 Hz for the unperturbed problem, but in the random case it is at 495 Hz for L ¼ 0.5 m and 490 Hz for L ¼ 5 m. This effect was also noticed for random roughness. 22 Besides, the agreement between the mean pressure computed with the Bourret approximation and by an ensemble-averaging over 200 realizations is satisfactory. In particular, for L ¼ 0.5 m, the curves depicting these two solutions are almost superimposed for both receiver heights.…”
Section: A Numerical Specificationmentioning
confidence: 70%
“…In acoustics, it has been used formerly to derive the average sound field or effective media quantities for multiple scattering problems, such as the propagation through a turbulent medium 4 or through a layer of scatterers. 21 Recently, based on this approach, Faure et al 22 have proposed an effective admittance to represent the reflection over rough surfaces.…”
Section: B Analytical Solution In the Fourier Spacementioning
confidence: 99%