TY - GEN
T1 - On Controlling the Path & Structure of a Leading-Edge Vortex by a Single, Small Jet
AU - Kalyankar, Harshad
AU - Noel, Alex Higuera Pierre
AU - Urreiztieta, Unai
AU - Taubert, Lutz
AU - Wygnanski, Israel
N1 - Publisher Copyright:
© 2025, American Institute of Aeronautics and Astronautics Inc, AIAA. All rights reserved.
PY - 2025
Y1 - 2025
N2 - The flow over a straight and a cranked lambda wing planform having a flat upper surface, and a sharp leading edge was investigated experimentally, using flow visualization and particle image velocimetry, while measuring the forces and moments on the model. A single steady jet located just inboard of the crank provided the wing with nose up or down pitch control authority and enabled the wing to be trimmed at high angles of incidence. To achieve this result the jet was rotated at various angles relative to the oncoming free stream therefore disrupting the feedback mechanism existing between the primary leading-edge vortex and the separated shear layer that feeds it with vorticity. In the absence of a crank, this feedback is provided by the vortical layer (secondary vortex) that is forced upward by the primary vortex and is entrained into the separated shear layer. In the presence of the crank, a new vortex created downstream of a crank serves a similar purpose as the shear layer. The experiments were carried out in a low-speed wind tunnel at 25 meters/second therefore providing a Reynold number of approximately 1.2 x 106 and a Mach number smaller than 0.1.
AB - The flow over a straight and a cranked lambda wing planform having a flat upper surface, and a sharp leading edge was investigated experimentally, using flow visualization and particle image velocimetry, while measuring the forces and moments on the model. A single steady jet located just inboard of the crank provided the wing with nose up or down pitch control authority and enabled the wing to be trimmed at high angles of incidence. To achieve this result the jet was rotated at various angles relative to the oncoming free stream therefore disrupting the feedback mechanism existing between the primary leading-edge vortex and the separated shear layer that feeds it with vorticity. In the absence of a crank, this feedback is provided by the vortical layer (secondary vortex) that is forced upward by the primary vortex and is entrained into the separated shear layer. In the presence of the crank, a new vortex created downstream of a crank serves a similar purpose as the shear layer. The experiments were carried out in a low-speed wind tunnel at 25 meters/second therefore providing a Reynold number of approximately 1.2 x 106 and a Mach number smaller than 0.1.
UR - https://www.scopus.com/pages/publications/105001404552
UR - https://www.scopus.com/pages/publications/105001404552#tab=citedBy
U2 - 10.2514/6.2025-1450
DO - 10.2514/6.2025-1450
M3 - Conference contribution
AN - SCOPUS:105001404552
SN - 9781624107238
T3 - AIAA Science and Technology Forum and Exposition, AIAA SciTech Forum 2025
BT - AIAA Science and Technology Forum and Exposition, AIAA SciTech Forum 2025
PB - American Institute of Aeronautics and Astronautics Inc, AIAA
T2 - AIAA Science and Technology Forum and Exposition, AIAA SciTech Forum 2025
Y2 - 6 January 2025 through 10 January 2025
ER -