Vortex Dynamic Investigation of Wing Slotted Gap of Saab Jas Gripen C-Like Fighter
Slamet Sutrisno, Setyawan Bekti Wibowo, Sigit Iswahyudi, Tri Agung Rohmat
Abstract
Slamet Sutrisno, Setyawan Bekti Wibowo, Sigit Iswahyudi, Tri Agung Rohmat
Abstract
Canard fighters generally configured with wing canard-deltas and would generate an airflow phenomenon producing vortex cores and lifts. The lift distribution would stall at a high angle of attack (AoA). This study investigated the vortex dynamic of wing canard delta configurations of the Saab JAS Gripen C-like model which create different wing planform than other fighters. The slotted leading edge of the Gripen would develop a strong vortex core on the outer wing, on the same direction with the spin of wing vortex; the outer core would drag the inner vortex core and strengthened. Consequently, the vortex core streamlined in a leading edge of the wing would begin to detach, resulting rolled-up vortices in the wing leading edge followed by a solid laminar stream which tends to curl out. The trailing edge of the wing tended to laminarize backward. The result would be a negative surface pressure on the leading edge above the canard and on the wing which causes more negative surface pressures. An increase in AoA will generate a closer vortex breakdown location to the wing leading edge. The location was calculated as the ratio of the axial velocity value to free velocity (U/U∞) at a value of 0.1. As the AoA increased, the vortex breakdown location moved forwards, upwards, and moved away from the fuselage.
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Canard fighters generally configured with wing canard-deltas and would generate an airflow phenomenon producing vortex cores and lifts. The lift distribution would stall at a high angle of attack (AoA). This study investigated the vortex dynamic of wing canard delta configurations of the Saab JAS Gripen C-like model which create different wing planform than other fighters. The slotted leading edge of the Gripen would develop a strong vortex core on the outer wing, on the same direction with the spin of wing vortex; the outer core would drag the inner vortex core and strengthened. Consequently, the vortex core streamlined in a leading edge of the wing would begin to detach, resulting rolled-up vortices in the wing leading edge followed by a solid laminar stream which tends to curl out. The trailing edge of the wing tended to laminarize backward. The result would be a negative surface pressure on the leading edge above the canard and on the wing which causes more negative surface pressures. An increase in AoA will generate a closer vortex breakdown location to the wing leading edge. The location was calculated as the ratio of the axial velocity value to free velocity (U/U∞) at a value of 0.1. As the AoA increased, the vortex breakdown location moved forwards, upwards, and moved away from the fuselage.
Key concepts: Vortex lift, Wing, Wingtip vortices, Vortex, Horseshoe vortex, Delta wing, Trailing edge, Angle of attack