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...

Full description

Bibliographic Details
Main Authors: Siwei Dong, Jianqiang Chen, Xianxu Yuan, Xi Chen, Guoliang Xu
Format: Article
Language:English
Published: SpringerOpen 2020-12-01
Series:Advances in Aerodynamics
Subjects:
Online Access:https://doi.org/10.1186/s42774-020-00057-4
id doaj-9d4e76a15e044e4895037b4e36358cd3
record_format Article
spelling 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 AT siweidong wallpressurebeneathatransitionalhypersonicboundarylayeroveraninclinedstraightcircularcone
AT jianqiangchen wallpressurebeneathatransitionalhypersonicboundarylayeroveraninclinedstraightcircularcone
AT xianxuyuan wallpressurebeneathatransitionalhypersonicboundarylayeroveraninclinedstraightcircularcone
AT xichen wallpressurebeneathatransitionalhypersonicboundarylayeroveraninclinedstraightcircularcone
AT guoliangxu wallpressurebeneathatransitionalhypersonicboundarylayeroveraninclinedstraightcircularcone
_version_ 1724376738395324416