10th Applied Aerodynamics Conference 1992
DOI: 10.2514/6.1992-2716
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Forebody vortex control for suppressing wing rock on a highly-swept wing configuration

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Cited by 13 publications
(7 citation statements)
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“…The primary causes of wing rock are the interactions between the forebody and the wing vortices at high angle of attack. 10 This has been verified using video-based experimental investigation for wing rock of sharp-edged delta wings with leading-edge sweep angles of 70 o and 80 o . 11 In order to predict roll divergence as well as other characteristics in the oscillation, a highly nonlinear analytical models of wing rock has been developed.…”
Section: Wing Rock Suppression Of Slender Delta Wingmentioning
confidence: 69%
“…The primary causes of wing rock are the interactions between the forebody and the wing vortices at high angle of attack. 10 This has been verified using video-based experimental investigation for wing rock of sharp-edged delta wings with leading-edge sweep angles of 70 o and 80 o . 11 In order to predict roll divergence as well as other characteristics in the oscillation, a highly nonlinear analytical models of wing rock has been developed.…”
Section: Wing Rock Suppression Of Slender Delta Wingmentioning
confidence: 69%
“…The primary causes of wing rock are the interactions between the forebody and the wing vortices at high angles of attack. 17 This has been verified using a video-based experimental investigation for wing rock of sharp-edged delta wings with leading-edge sweep angles of 70°and 80°, which also suggests that the limit cycle behavior is due to the relative phasing between model oscillations and vortex movements. 18 Analytical models of this highly nonlinear phenomenon have been developed and used to predict roll divergence as well as other characteristics in the oscillations, such as the period and amplitude of the oscillations.…”
Section: Wing Rock Suppressionmentioning
confidence: 70%
“…Ng and Malcolm used forebody strakes 57 and steady blowing and suction 52 over a slender delta wing (Ã ¼ 78 ) space-plane model and found that the wing rock can be suppressed by relocating or altering the strength of the forebody vortices. A similar space-plane model was also studied by Suarez et al, 53 who discovered that by applying pulse-blowing with frequency, that is, 2-3 times the wing rock frequency, optimum attenuation can be achieved. Moreover, the full length tangential leading-edge blowing on a double delta configuration was tested by Wong et al 54 It emerged that the blowing technique effectively altered the position and strength of the leading-edge vortices and hence the roll oscillations were suppressed at high angle of attack.…”
Section: Control Of Slender Wing Rockmentioning
confidence: 83%
“…As aforementioned, self-induced roll oscillations can occur in various LAR planforms regardless of whether they are delta or non-delta, slender or nonslender planforms. Earlier studies focused on suppressing the roll oscillations of slender delta wings and regarding these, both active [52][53][54][55][56] and passive [57][58][59][60] flow control techniques were applied. Ng and Malcolm used forebody strakes 57 and steady blowing and suction 52 over a slender delta wing (Ã ¼ 78 ) space-plane model and found that the wing rock can be suppressed by relocating or altering the strength of the forebody vortices.…”
Section: Control Of Slender Wing Rockmentioning
confidence: 99%