Numerical analysis of high speed wind tunnel flow disturbance measurements using stagnation point probes

Since supersonic test facilities have tunnel noise that strongly influences boundary layer transition experiments, the determination of tunnel noise is of great significance to properly evaluate and interpret experimental results. The composition of tunnel noise, which consists of acoustic, entropy and vorticity modes, highly influences the boundary layer receptivity. The measurement of the separate modes is a major goal of ongoing research. In this study, the properties of stagnation point probes for a newly developed modal decomposition method for tunnel noise are investigated by direct numerical simulation. Pressure and heat flux responses of a stagnation point probe to various entropy and acoustic mode input functions are analysed to investigate how tunnel noise is perceived by corresponding sensor types. The interaction of the incident mode and the shock wave upstream of the probe is analysed and the resulting wave pattern in the subsonic region between shock wave and probe is evidenced. It is found that pure incident acoustic or entropy modes cause acoustic and entropy waves downstream of the shock wave whose strengths differ depending on the incident mode. The resulting wave pattern downstream of the shock wave is determined by postshock acoustic waves propagating bidirectionally between shock wave and probe. Formulating a model equation linking pressure and heat flux fluctuations to the initially caused postshock acoustic and entropy wave, a criterion for the applicability of stagnation point probes measuring pressure and heat flux fluctuations in the new modal decomposition method can be deduced: to distinguish between the incident mode types based on their pressure and heat flux signal the perception of initially generated entropy waves downstream of the shock wave by the heat flux sensor is crucial. The transfer function between entropy waves and heat flux is shown to have low pass filter characteristics and the cutoff Strouhal number could be estimated by control theory. The analysis of the frequency response to continuous incident waves corroborated this cutoff Strouhal number.

[1]  Andreas Lintermann,et al.  Massively parallel grid generation on HPC systems , 2014 .

[2]  A. Maslov,et al.  Novel Sensor for Fast Heat Flux Measurements , 2009 .

[3]  S. Schneider Effects of Roughness on Hypersonic Boundary-Layer Transition , 2007 .

[4]  Wolfgang Schröder,et al.  An accurate moving boundary formulation in cut-cell methods , 2013, J. Comput. Phys..

[5]  J. C. Anyiwo,et al.  Turbulence amplification in shock-wave boundary-layer interaction , 1982 .

[6]  J. Laufer,et al.  Aerodynamic noise in supersonic wind tunnels , 1961 .

[7]  Xiaolin Zhong,et al.  Receptivity of a supersonic boundary layer over a flat plate. Part 3. Effects of different types of free-stream disturbances , 2005, Journal of Fluid Mechanics.

[8]  Steven P. Schneider,et al.  Effects of High-Speed Tunnel Noise on Laminar-Turbulent Transition , 2000 .

[9]  A. Fedorov Transition and Stability of High-Speed Boundary Layers , 2011 .

[10]  O. Chazot,et al.  Flow characterization and boundary layer transition studies in {VKI} hypersonic facilities , 2015 .

[11]  R. Radespiel,et al.  Disturbance-Level and Transition Measurements in a Conical Boundary Layer at Mach 6 , 2008 .

[12]  Olivier Chazot,et al.  Disturbance Level Characterization of a Hypersonic Blowdown Facility , 2012 .

[13]  W. R. Grabowsky,et al.  The search for optimum configurations for re-entry vehicles , 1984 .

[14]  Wolfgang Schröder,et al.  Analysis of acoustic and entropy disturbances in a hypersonic wind tunnel , 2016 .

[15]  A. J. Laderman,et al.  Mean and fluctuating flow measurements in the hypersonic boundary layer over a cooled wall , 1974, Journal of Fluid Mechanics.

[16]  P. Logan Modal analysis of hot-wire measurements in supersonic turbulence , 1988 .

[17]  S. M. Derry,et al.  Review of boundary layer transition flight data on the Space Shuttle Orbiter , 1991 .

[18]  L. Kovasznay Turbulence in Supersonic Flow , 1953 .

[19]  Wolfgang Schröder,et al.  Cut-cell method based large-eddy simulation of tip-leakage flow , 2015 .

[20]  J. F. Mckenzie,et al.  Interaction of Linear Waves with Oblique Shock Waves , 1968 .

[21]  K. E. Wurster An assessment of the impact of transition on advanced winged entry vehicle thermal protection system mass , 1981 .

[22]  E. Reshotko Boundary layer instability, transition and control , 1994 .

[23]  Xiaolin Zhong,et al.  Receptivity of a supersonic boundary layer over a flat plate. Part 1. Wave structures and interactions , 2003, Journal of Fluid Mechanics.

[24]  X. Zhong,et al.  Direct Numerical Simulation on the Receptivity, Instability, and Transition of Hypersonic Boundary Layers , 2012 .

[25]  Xiaolin Zhong,et al.  Receptivity of a supersonic boundary layer over a flat plate. Part 2. Receptivity to free-stream sound , 2003, Journal of Fluid Mechanics.

[26]  S. Schneider Summary of Hypersonic Boundary-Layer Transition Experiments on Blunt Bodies with Roughness , 2008 .

[27]  M. V. Morkovin,et al.  Note on the Assessment of Flow Disturbances at a Blunt Body Traveling at Supersonic Speeds Owing to Flow Disturbances in Free Stream , 1960 .

[28]  D. Hartmann,et al.  An adaptive multilevel multigrid formulation for Cartesian hierarchical grid methods , 2008 .

[29]  A. Fedorov,et al.  Receptivity of a high-speed boundary layer to temperature spottiness , 2013, Journal of Fluid Mechanics.

[30]  Alexander Fedorov,et al.  Receptivity of a high-speed boundary layer to acoustic disturbances , 2003, Journal of Fluid Mechanics.

[31]  E. Reshotko,et al.  Stability of the Laminar Boundary Layer on a Blunted Plate in Supersonic Flow , 1980 .

[32]  Rolf Radespiel,et al.  Flow quality experiment in a tandem nozzle wind tunnel at Mach 3 , 2015 .

[33]  Shann J. Rufer,et al.  Unsteady heat-flux measurements of second-mode instability waves in a hypersonic flat-plate boundary layer , 2015, Experiments in fluids.