Patterns and prediction of surface peak heat flux in hypersonic flat plate boundary layer over wave wall

被引:0
作者
Kong X. [1 ]
Han Y. [1 ]
机构
[1] Laboratory for High-Speed Aerodynamics, Tianjin University, Tianjin
来源
Hangkong Xuebao/Acta Aeronautica et Astronautica Sinica | 2023年 / 44卷 / 12期
关键词
aerodynamic heat; hypersonic; peak heat flux; predictive model; rough wall;
D O I
10.7527/S1000-6893.2022.27769
中图分类号
学科分类号
摘要
Micro ablation on the surface of new-type vehicles will lead to increased local heat flux on the wall surface. This study uses corrugated roughness with roughness height smaller than 600 μm to simulate micro ablative surfaces,and calculates the variation law of the peak heat flux on the wall surface with uniform corrugated roughness by directly solving the Navier-Stokes equation. It is found that the surface peak heat flux caused by roughness is inversely propor⁃ tional to the 0. 5 times of the flow position,the surface peak heat flux is proportional to the roughness height and de⁃ creases with increasing width,and is more influenced by the height than the width. Meanwhile,the influence results of the Mach number and wall temperature on the surface peak heat flux at the wall show that the relative surface peak heat flux increment is inversely proportional to both the Mach number and wall temperature. Further,based on the smooth flat plate heat flux theory solution,we provide the surface peak heat flux prediction formula. Detailed verifica⁃ tion of the working conditions reveals that the formula can accurately predict the surface peak heat flux in the range of Mach number 4-10 and wall temperature 300-800 K with an error of no more than 8%. For other wall forms,such as elliptical and dispersive sine types,the formula can also produce an accurate prediction. © 2023 AAAS Press of Chinese Society of Aeronautics and Astronautics. All rights reserved.
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共 28 条
[1]  
WHITE C M., Experiments with fluid friction in roughened pipes[J], Proceedings of the Royal Society of London Series A-Mathematical and Physical Sciences, 161, 906, pp. 367-381, (1937)
[2]  
SCHLICHTING H., Experimentelle untersuchungen zum rauhigkeitsproblem[J], Ingenieur-Archiv, 7, 1, pp. 1-34, (1936)
[3]  
NIKURADSE J., Laws of flow in rough pipes:Technical Memorandum 1292[R], (1950)
[4]  
SIGAL A, DANBERG J E., New correlation of roughness density effect on the turbulent boundary layer[J], AIAA Journal, 28, 3, pp. 554-556, (1990)
[5]  
DE MARCHIS M., The ef⁃ fect of the slope of irregularly distributed roughness ele⁃ ments on turbulent wall-bounded flows [J], Journal of Fluid Mechanics, 613, pp. 385-394, (2008)
[6]  
DONG C., Several key issues in the aerodynamic design of hypersonic ve⁃ hicles [J], Science in China: Physics Mechanics As⁃ tronomy, 51, 10, pp. 2-21
[7]  
BERTRAM M,, WEINSTEIN L, Et al., Heat transfer to wavy wall in hypersonic flow[J], AIAA Journal, 5, 10, pp. 1760-1767, (1967)
[8]  
JAECK C L., Analysis of pressure and heat transfer tests on surface roughness elements with laminar and turbulent boundary layers[M], (1966)
[9]  
COOPER L,, Et al., Passive Nosetip Technology (PANT) Program. Vol⁃ ume 20. Investigation of flow phenomena over reentry vehicle nosetips[R], (1975)
[10]  
STOKES T., The effect of transition and boundary layer development on hyper⁃ sonic reentry shape change, 10th Thermophysics Conference, (1975)