Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone
Abstract Properties of wall pressure beneath a transitional hypersonic boundary layer over a 7∘ half-angle blunt cone at angle of attack 6∘ are studied by Direct Numerical Simulation. The wall pressure has two distinct frequency peaks. The low-frequency peak with f≈10−50 kHz is very likely the unste...
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Online Access: | https://doi.org/10.1186/s42774-020-00057-4 |
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doaj-9d4e76a15e044e4895037b4e36358cd32020-12-20T12:18:32ZengSpringerOpenAdvances in Aerodynamics2524-69922020-12-012112010.1186/s42774-020-00057-4Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular coneSiwei Dong0Jianqiang Chen1Xianxu Yuan2Xi Chen3Guoliang Xu4State Key Laboratory of Aerodynamics, China Aerodynamics Research and Development CenterState Key Laboratory of Aerodynamics, China Aerodynamics Research and Development CenterState Key Laboratory of Aerodynamics, China Aerodynamics Research and Development CenterState Key Laboratory of Aerodynamics, China Aerodynamics Research and Development CenterState Key Laboratory of Aerodynamics, China Aerodynamics Research and Development CenterAbstract Properties of wall pressure beneath a transitional hypersonic boundary layer over a 7∘ half-angle blunt cone at angle of attack 6∘ are studied by Direct Numerical Simulation. The wall pressure has two distinct frequency peaks. The low-frequency peak with f≈10−50 kHz is very likely the unsteady crossflow mode based on its convection direction, i.e. along the axial direction and towards the windward symmetry ray. High-frequency peaks are roughly proportional to the local boundary layer thickness. Along the trajectories of stationary crossflow vortices, the location of intense high-frequency wall pressure moves from the bottom of trough where the boundary layer is thin to the bottom of shoulder where the boundary layer is thick. By comparing the pressure field with that inside a high-speed transitional swept-wing boundary layer dominated by the z-type secondary crossflow mode, we found that the high-frequency signal originates from the Mack mode and evolves into the secondary crossflow instability.https://doi.org/10.1186/s42774-020-00057-4Wall pressureMack modeSecondary crossflow instabilityInclined cone |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Siwei Dong Jianqiang Chen Xianxu Yuan Xi Chen Guoliang Xu |
spellingShingle |
Siwei Dong Jianqiang Chen Xianxu Yuan Xi Chen Guoliang Xu Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone Advances in Aerodynamics Wall pressure Mack mode Secondary crossflow instability Inclined cone |
author_facet |
Siwei Dong Jianqiang Chen Xianxu Yuan Xi Chen Guoliang Xu |
author_sort |
Siwei Dong |
title |
Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
title_short |
Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
title_full |
Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
title_fullStr |
Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
title_full_unstemmed |
Wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
title_sort |
wall pressure beneath a transitional hypersonic boundary layer over an inclined straight circular cone |
publisher |
SpringerOpen |
series |
Advances in Aerodynamics |
issn |
2524-6992 |
publishDate |
2020-12-01 |
description |
Abstract Properties of wall pressure beneath a transitional hypersonic boundary layer over a 7∘ half-angle blunt cone at angle of attack 6∘ are studied by Direct Numerical Simulation. The wall pressure has two distinct frequency peaks. The low-frequency peak with f≈10−50 kHz is very likely the unsteady crossflow mode based on its convection direction, i.e. along the axial direction and towards the windward symmetry ray. High-frequency peaks are roughly proportional to the local boundary layer thickness. Along the trajectories of stationary crossflow vortices, the location of intense high-frequency wall pressure moves from the bottom of trough where the boundary layer is thin to the bottom of shoulder where the boundary layer is thick. By comparing the pressure field with that inside a high-speed transitional swept-wing boundary layer dominated by the z-type secondary crossflow mode, we found that the high-frequency signal originates from the Mack mode and evolves into the secondary crossflow instability. |
topic |
Wall pressure Mack mode Secondary crossflow instability Inclined cone |
url |
https://doi.org/10.1186/s42774-020-00057-4 |
work_keys_str_mv |
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