2007
DOI: 10.1016/j.apacoust.2005.10.004
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Time-domain calculations of sound interactions with outdoor ground surfaces

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Cited by 41 publications
(39 citation statements)
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“…At this high-Reynolds number, a relatively broad spectrum of pressure fluctuations is generated with flow over the upstream circular cylinder, in contrast to a low-Reynolds number flow, where only very tonal pressure fluctuations, related to the von Karman vortex shedding frequency, are generated. The shape of the broadband spectrum of the unscreened case (to be shown shortly) is very similar to those of wind noise in the literature [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] that follow the À5/3-frequency power decay of the spectrum of atmospheric turbulent pressure.…”
Section: Resultssupporting
confidence: 64%
See 1 more Smart Citation
“…At this high-Reynolds number, a relatively broad spectrum of pressure fluctuations is generated with flow over the upstream circular cylinder, in contrast to a low-Reynolds number flow, where only very tonal pressure fluctuations, related to the von Karman vortex shedding frequency, are generated. The shape of the broadband spectrum of the unscreened case (to be shown shortly) is very similar to those of wind noise in the literature [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] that follow the À5/3-frequency power decay of the spectrum of atmospheric turbulent pressure.…”
Section: Resultssupporting
confidence: 64%
“…The resulting momentum equation for air flow inside the windscreen is the ZK equation, 11 which is the low-frequency limit of more general forms of porous media equations. 19 In addition, incompressibility is assumed for flow inside the porous medium. The convection and diffusion terms are neglected in the original ZK equation because the velocity is low in the porous medium.…”
Section: Formulation and Solution Schemesmentioning
confidence: 99%
“…Only when there is interest in predicting the attenuation inside the porous medium at high sound frequencies and low flow resistivities, adaptions should be made as presented in [21]. Note, however, that the UWVF model is not restricted to a particular porous model, and other models can be implemented without additional difficulties.…”
Section: Equations For Sound Propagation In Porous Mediamentioning
confidence: 99%
“…The porosity, structure factor and flow resistivity of the barrier are chosen as 0.4, 1.35 and 50k Pa·s/m 2 , respectively. Although no particular material is aimed at, such a set of parameters could be representative for uncompacted earth [26,21]. In the UWVF method, the largest allowed mesh size of 0.68 m is used, which is twice the wave length which equals 0.34 m when using a speed of sound of 340 m/s.…”
Section: Sound Propagation Near a Porous Barriermentioning
confidence: 99%
“…The air flow inside the windscreen is modeled with the ZK equation, 3 which is the low-frequency limit of more general forms of porous media equations. 11 In addition, incompressibility is assumed for flow inside the porous medium. The governing equations for airflow inside the windscreen are expressed in Eq.…”
Section: Formulation and Numerical Schemesmentioning
confidence: 99%