“…For downwind the results show that the insertion loss fluctuates around zero. This is in agreement with findings of Scholes et al 16 who measured the influence of screens ͑full scale measurements͒ and who found that in a downwind situation the insertion loss was not always positive.…”
Section: B Comparison With Acoustical Data From Scale Modelsupporting
confidence: 93%
“…In practice the insertion loss will often be influenced by temperature gradients and wind, including turbulence effects, but it appears that only few studies of this exist. [15][16][17][18][19] In the present work a screen on a finite impedance surface representative of grass-covered ground is investigated experimentally and theoretically under the influence of wind. Upwind as well as downwind conditions are investigated.…”
Point source propagation over a screen located on a finite impedance surface representative of grass-covered ground is investigated under upwind and downwind conditions. The theoretical part of the investigation involves extended use of parabolic equation methods ͑PE͒ allowing for the changes in the vertical wind speed profile when the wind field passes the screen. The influence of turbulence is also implemented. The experimental part of the investigation relies on a scale model technique based upon a 1:25 scaling ratio and a triggered spark source. The main results relate to the size of the insertion loss of a screen under windy conditions and to the acoustic importance of the redirection of the flow before and after the screen.
“…For downwind the results show that the insertion loss fluctuates around zero. This is in agreement with findings of Scholes et al 16 who measured the influence of screens ͑full scale measurements͒ and who found that in a downwind situation the insertion loss was not always positive.…”
Section: B Comparison With Acoustical Data From Scale Modelsupporting
confidence: 93%
“…In practice the insertion loss will often be influenced by temperature gradients and wind, including turbulence effects, but it appears that only few studies of this exist. [15][16][17][18][19] In the present work a screen on a finite impedance surface representative of grass-covered ground is investigated experimentally and theoretically under the influence of wind. Upwind as well as downwind conditions are investigated.…”
Point source propagation over a screen located on a finite impedance surface representative of grass-covered ground is investigated under upwind and downwind conditions. The theoretical part of the investigation involves extended use of parabolic equation methods ͑PE͒ allowing for the changes in the vertical wind speed profile when the wind field passes the screen. The influence of turbulence is also implemented. The experimental part of the investigation relies on a scale model technique based upon a 1:25 scaling ratio and a triggered spark source. The main results relate to the size of the insertion loss of a screen under windy conditions and to the acoustic importance of the redirection of the flow before and after the screen.
“…Comparing the frequency spectrum of reflection theory of a point source of HNP 1.0 with that ofTNM 2.5 and the measurements by Parkin and Scholes (Parkin, 1965) 2. Comparing the frequency spectrum of insertion loss of a point source of HNP 1.0 with that ofTNM 2.5 and the measurements by Scholes (Scholes, 1971) 3. Comparing the insertion loss at receiver points by a line source ofHNP 1.0 with that of TNM 2.5 and STAMINA 2.…”
Section: Research Objectivesmentioning
confidence: 99%
“…The second verification is to compare ground effect with the measurements by Parkin and Scholes over grassland (Parkin, 1965). The third verification is to compare the insertion loss of a noise barrier by Scholes, also over grassland (Scholes, 1971). Since TNM validations are mainly based on the above three verification cases of point source, HNP will also provide detailed comparisons for all these cases.…”
Section: Verification Oftnm Validation Cases With a Point Sourcementioning
confidence: 99%
“…conducted TNM validation by comparing the TNM predicted insertion loss with the measured barrier insertion loss of Scholes (Scholes 1971) using the point source. The comparisons were made with a limited set of measured data with the following geometry: source height of 0.7 m (2.3 ft); barrier heights of 1.8 m (6 ft) and 4.9 m (16 ft); microphone heights of 1.5 m (5 ft), 3 m (10 ft), 6 m (20 ft) and 12 m (40 ft), source-to-barrier distance of 10 m (33 ft); and barrier to receiver distance of30 m (100 ft).…”
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