16th AIAA/CEAS Aeroacoustics Conference 2010
DOI: 10.2514/6.2010-3803
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Experimental Investigation of Airfoil Self Noise and Turbulent Wake Reduction by the use of Trailing Edge Serrations

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Cited by 88 publications
(79 citation statements)
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“…This can be explained by the fact that the characteristic time scale of a vortex moving past the sharp leading edge is several orders of magnitude smaller than the integral time scale of the turbulence. This would need however to be re-examined for realistic airfoils where the leading edge has a finite radius of curvature, for instance using experimental data from Paterson & Amiet [35], Devenport et al [36] or Gruber & Joseph [37,38]. Note that although all the validation examples presented here are against analytical solutions, comparisons with experimental data have been presented in [20], but they were not sufficiently conclusive as far as the effect of the integral time scale is concerned, mainly because the numerical simulations were using a flat plate.…”
Section: Discussionmentioning
confidence: 99%
“…This can be explained by the fact that the characteristic time scale of a vortex moving past the sharp leading edge is several orders of magnitude smaller than the integral time scale of the turbulence. This would need however to be re-examined for realistic airfoils where the leading edge has a finite radius of curvature, for instance using experimental data from Paterson & Amiet [35], Devenport et al [36] or Gruber & Joseph [37,38]. Note that although all the validation examples presented here are against analytical solutions, comparisons with experimental data have been presented in [20], but they were not sufficiently conclusive as far as the effect of the integral time scale is concerned, mainly because the numerical simulations were using a flat plate.…”
Section: Discussionmentioning
confidence: 99%
“…Lyu et al 13 further developed a new semi-analytical model applying the Schwarzschild method of propagation of the pressure fluctuations. Although closer to reality, the final result does not allow yet to explain some of the physical features already at zero angle of attack such as the characteristic cross-over frequency St δ = fδ/V ∞ ≈ 1 (based on the free-stream velocity V ∞ and boundary-layer thickness δ, from XFOIL) 14 after which noise increases again. It was recently showed that one of the limitation of the theoretical model is the assumption of frozen turbulence along the serration length.…”
Section: Introductionmentioning
confidence: 99%
“…The model predicts an asymptotic noise reduction value at high frequency of 10log 10 [1 + (4h/b) 2 overestimates the magnitude of the noise reduction with serration add-ons. Moreover, the model is not suitable for predicting the characteristic frequency St δ = f δ/U ∞ ≈ 1 (based on the free-stream velocity U ∞ and boundary layer thickness δ estimated with XFOIL in the study of Gruber et al 26 ) after which noise increases again.…”
Section: Introductionmentioning
confidence: 99%
“…It may also clarify the discrepancies between measured and predicted noise reduction reported in previous studies. Until now, a link between flow measurements 13,26,36 and their aeroacoustics footprint is missing. Clemons and Wlezien 36 used hot-wire anemometry to measure the convective velocity and spanwise correlation length of the streamwise velocity turbulent fluctuations.…”
mentioning
confidence: 99%