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Large-eddy simulation of shock-wave/turbulent boundary layer interaction with and without Spark Jet control 被引量:9

Large-eddy simulation of shock-wave/turbulent boundary layer interaction with and without Spark Jet control
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摘要 The efficiency and mechanism of an active control device "'Spark Jet" and its application in shock-induced separation control are studied using large-eddy simulation in this paper. The base flow is the interaction of an oblique shock-wave generated by 8° wedge and a spatially-developing Ma = 2.3 turbulent boundary layer. The Reynolds number based on the incoming flow property and the boundary layer displacement thickness at the impinging point without shock-wave is 20000. The detailed numerical approaches were presented. The inflow turbulence was generated using the digital filter method to avoid artificial temporal or streamwise periodicity. The , merical results including velocity profile, Reynolds stress profile, skin friction, and wall pressure were sys- tematically validated against the available wind tunnel particle image velocimetry (PIV) measure- ments of the same flow condition. Further study on the control of flow separation due to the strong shock-viscous interaction using an active control actuator "'Spark Jet'" was conducted. The single-pulsed characteristic of the device was obtained and compared with the experiment. Both instantaneous and time-averaged flow fields have shown that the jet flow issuing from the actuator cavity enhances the flow mixing inside the boundary layer, making the boundary layer more resis- tant to flow separation. Skin friction coefficient distribution shows that the separation bubble length is reduced by about 35% with control exerted. The efficiency and mechanism of an active control device "'Spark Jet" and its application in shock-induced separation control are studied using large-eddy simulation in this paper. The base flow is the interaction of an oblique shock-wave generated by 8° wedge and a spatially-developing Ma = 2.3 turbulent boundary layer. The Reynolds number based on the incoming flow property and the boundary layer displacement thickness at the impinging point without shock-wave is 20000. The detailed numerical approaches were presented. The inflow turbulence was generated using the digital filter method to avoid artificial temporal or streamwise periodicity. The , merical results including velocity profile, Reynolds stress profile, skin friction, and wall pressure were sys- tematically validated against the available wind tunnel particle image velocimetry (PIV) measure- ments of the same flow condition. Further study on the control of flow separation due to the strong shock-viscous interaction using an active control actuator "'Spark Jet'" was conducted. The single-pulsed characteristic of the device was obtained and compared with the experiment. Both instantaneous and time-averaged flow fields have shown that the jet flow issuing from the actuator cavity enhances the flow mixing inside the boundary layer, making the boundary layer more resis- tant to flow separation. Skin friction coefficient distribution shows that the separation bubble length is reduced by about 35% with control exerted.
出处 《Chinese Journal of Aeronautics》 SCIE EI CAS CSCD 2016年第3期617-629,共13页 中国航空学报(英文版)
基金 supported by the National Natural Science Foundation of China(Nos.11302012,51420105008,51476004,11572025 and 51136003) the National Basic Research Program of China(No.2012CB720205) The computational time for the present study was provided by the UK Turbulence Consortium(EPSRC grant EP/L000261/1)
关键词 Large-eddy simulation Shock-wave:Turbulent boundary layer INTERACTION Spark Jet control Large-eddy simulation Shock-wave:Turbulent boundary layer Interaction Spark Jet control
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