13th Aeroacoustics Conference 1990
DOI: 10.2514/6.1990-4009
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Effect of acoustic excitation on stalled flows over an airfoil

Abstract: The effect of acoustic excitation on poststalled flows over an airfoil, i.e., flows that are fully separated from near the leading edge, is investigated. The excitation results in a tendency towards reattachment, which is accompanied by an increased lift and reduced drag, although the flow may still remain fully separated. It is found that with increasing excitation amplitude, the effect becomes more pronounced but shifts to a Strouhal number which is much lower than that expected from linear, inviscid instabi… Show more

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Cited by 9 publications
(15 citation statements)
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“…At Rea = 7.7 • 104 it was found that maximum attenuation occurred at the excitation frequency rex = 2.5 kHz. This excitation frequency agreed with that on airfoil McKinzie 1991 andZaman 1992). At Rea= 1.22 x 105 fex for maximum attenuation was 2.3 kHz.…”
Section: Apparatus and Measurement Techniquesupporting
confidence: 73%
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“…At Rea = 7.7 • 104 it was found that maximum attenuation occurred at the excitation frequency rex = 2.5 kHz. This excitation frequency agreed with that on airfoil McKinzie 1991 andZaman 1992). At Rea= 1.22 x 105 fex for maximum attenuation was 2.3 kHz.…”
Section: Apparatus and Measurement Techniquesupporting
confidence: 73%
“…At this Reynolds number the momentum thickness 0is at the laminar separation point was found to be 0.1438 mm, giving the Strouhal number Sto( =fex 0is/Uo) of 0.015. This is very near the Strouhal number of about 0.016, when rex matches the instability frequency of the separated shear layer (Zaman 1992). The excitation level, as measured on the tunnel wall, was 120 dB.…”
Section: Apparatus and Measurement Techniquementioning
confidence: 95%
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“…Combined with the result of [4], we can find the importance of large scale vortex in interaction between sound and vortex. In [5], the phenomena that the effect of the sound on the lower stream flow is small is related with isotropy of the lower stream vortex: which is nearly consistent. In [6] the pressure amplitude is also large at fi= 1220Hz.…”
Section: 4 Pl=aexp[i(-koy-co~t) ] Vl-=~ocoexp[i(-koy-cot) ]supporting
confidence: 56%
“…There exists free shear layer over the separated area on the stalled flow of the airfoil in [5]. [6], so the perturbation equations developed above can be applied.…”
Section: Interaction Between First Order Sound and Vortex And Creatimentioning
confidence: 99%