TY - GEN
T1 - Laminar-Turbulent Transition in a Swept Low-Speed Boundary Layer
AU - Bahrainirad, Ladan
AU - Hosseinverdi, Shirzad
AU - Fasel, Hermann F.
N1 - Publisher Copyright:
© 2022, American Institute of Aeronautics and Astronautics Inc, AIAA. All rights reserved.
PY - 2022
Y1 - 2022
N2 - Evolution of three-dimensional disturbances in an accelerating swept laminar boundary layer is investigated by direct numerical simulations and linear parabolized stability equations (PSE). First, so-called controlled transition simulations were carried out where a single unsteady secondary instability wave is added to the baseflow distorted by a stationary primary crossflow vortex, and the nature of secondary instability regimes was identified. Next, the development of a three-dimensional wave packet was investigated, where the wave packet is generated by a localized short-duration pulse disturbance. DNS data support the results obtained from a PSE analysis, namely that the underlying baseflow is unstable with respect to both stationary and traveling crossflow modes with a wide range of frequencies and spanwise wavenumbers, whereby traveling crossflow modes are reaching the largest maximum amplitudes. Nonlinear mechanisms eventually trigger the transition process, as the wave packet breakdown to turbulent patches.
AB - Evolution of three-dimensional disturbances in an accelerating swept laminar boundary layer is investigated by direct numerical simulations and linear parabolized stability equations (PSE). First, so-called controlled transition simulations were carried out where a single unsteady secondary instability wave is added to the baseflow distorted by a stationary primary crossflow vortex, and the nature of secondary instability regimes was identified. Next, the development of a three-dimensional wave packet was investigated, where the wave packet is generated by a localized short-duration pulse disturbance. DNS data support the results obtained from a PSE analysis, namely that the underlying baseflow is unstable with respect to both stationary and traveling crossflow modes with a wide range of frequencies and spanwise wavenumbers, whereby traveling crossflow modes are reaching the largest maximum amplitudes. Nonlinear mechanisms eventually trigger the transition process, as the wave packet breakdown to turbulent patches.
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U2 - 10.2514/6.2022-3633
DO - 10.2514/6.2022-3633
M3 - Conference contribution
AN - SCOPUS:85135071150
SN - 9781624106354
T3 - AIAA AVIATION 2022 Forum
BT - AIAA AVIATION 2022 Forum
PB - American Institute of Aeronautics and Astronautics Inc, AIAA
T2 - AIAA AVIATION 2022 Forum
Y2 - 27 June 2022 through 1 July 2022
ER -