TY - GEN
T1 - Experimental and computational results of a cone-slice-ramp geometry at mach 6
AU - Vogel, Ethan A.
AU - Coder, James G.
AU - Chynoweth, Brandon C.
AU - Schneider, Steven P.
N1 - Publisher Copyright:
© 2019, American Institute of Aeronautics and Astronautics Inc, AIAA. All rights reserved.
PY - 2019
Y1 - 2019
N2 - Experiments were performed in the Boeing/AFOSR Mach-6 Quiet Tunnel on a cone-slice-ramp geometry. The cone half-angle was 9◦ . Ramp angles of 5◦, 10◦, 20◦, and 30◦ from the centerline of the model were tested at a unit Reynolds number of 11.3×106 /m. Computations were performed at similar conditions using the NASA OVERFLOW solver. With the 5◦ and 10◦ ramps under quiet flow conditions, experiments measure three streamwise streaks of heating on the slice. These streaks do not occur with the 20◦ and 30◦ ramps. Surface pressure sensors measure disturbances for several conditions on the slice and ramp, but it currently cannot be determined experimentally if the flow is laminar or dominated by large separated regions. Under noisy flow, two large turbulent wedges develop on the slice region for all four ramp angles. The turbulent boundary layer remains attached when the flow encounters the ramp. Three streaks are also computed for ramp deflection angles of 10◦, 20◦, and 30◦ . The 5◦ case has not been computed. The cause of the discrepancy in the number of streaks on the slice for the 20◦ and 30◦ cases is being investigated. On the deflected ramp surface, similar heating rates and patterns occur in the computations and experiments.
AB - Experiments were performed in the Boeing/AFOSR Mach-6 Quiet Tunnel on a cone-slice-ramp geometry. The cone half-angle was 9◦ . Ramp angles of 5◦, 10◦, 20◦, and 30◦ from the centerline of the model were tested at a unit Reynolds number of 11.3×106 /m. Computations were performed at similar conditions using the NASA OVERFLOW solver. With the 5◦ and 10◦ ramps under quiet flow conditions, experiments measure three streamwise streaks of heating on the slice. These streaks do not occur with the 20◦ and 30◦ ramps. Surface pressure sensors measure disturbances for several conditions on the slice and ramp, but it currently cannot be determined experimentally if the flow is laminar or dominated by large separated regions. Under noisy flow, two large turbulent wedges develop on the slice region for all four ramp angles. The turbulent boundary layer remains attached when the flow encounters the ramp. Three streaks are also computed for ramp deflection angles of 10◦, 20◦, and 30◦ . The 5◦ case has not been computed. The cause of the discrepancy in the number of streaks on the slice for the 20◦ and 30◦ cases is being investigated. On the deflected ramp surface, similar heating rates and patterns occur in the computations and experiments.
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U2 - 10.2514/6.2019-3593
DO - 10.2514/6.2019-3593
M3 - Conference contribution
AN - SCOPUS:85092413301
SN - 9781624105890
T3 - AIAA Aviation 2019 Forum
SP - 1
EP - 18
BT - AIAA Aviation 2019 Forum
PB - American Institute of Aeronautics and Astronautics Inc, AIAA
T2 - AIAA Aviation 2019 Forum
Y2 - 17 June 2019 through 21 June 2019
ER -