Fluid Mechanics and Flight Mechanics

Research on Ablation for Crew Return Vehicle Based on Re-entry Trajectory and Aerodynamic Heating Environment

  • WANG Jun ,
  • PEI Hailong ,
  • WANG Naizhou
Expand
  • 1. Key Laboratory of Autonomous Systems and Networked Control, Ministry of Education, South China University of Technology, Guangzhou 510640, China;
    2. School of Automation Science and Engineering, South China University of Technology, Guangzhou 510640, China

Received date: 2013-02-14

  Revised date: 2013-03-11

  Online published: 2013-03-19

Supported by

National Natural Science Foundation of China (61174053);Research Fund for the Doctoral Program of Higher Education of China (20100172110023)

Abstract

The ablation of a heat shield subjected to dynamic changes of the surface material depth and temperature can be reasonably predicted in the whole re-entry process. The approach of constructing a dynamic ablation process is presented by combining the reentry trajectory and aerodynamic heat with Newton-Raphson and tridiagonal matrices (TDMA) algorithms. A three degrees of freedom direct and skip re-entry trajectory model is established. The modified Newtonian flow theory,Fay-Riddell and Sutton-Grave theory are adopted to calculate respectively the aerodynamic parameters and stagnation heat flux. A one dimensional nonlinear heat conduction model is employed to simulate the process of thermal protective material ablation. The results of ablation prediction demonstrate that continuous dynamic change of the surface material depth and the temperature can be realized. The proposed method can be applied to more complicated structures of the flight vehicles and the results of it are shown to be reliable and reasonable by comparing them with those of the heat balance integral (HBI) method. This study provides a reference for further optimization of the design of thermal protection systems (TPS).

Cite this article

WANG Jun , PEI Hailong , WANG Naizhou . Research on Ablation for Crew Return Vehicle Based on Re-entry Trajectory and Aerodynamic Heating Environment[J]. ACTA AERONAUTICAET ASTRONAUTICA SINICA, 2014 , 35(1) : 80 -89 . DOI: 10.7527/S1000-6893.2013.0167

References

[1] Greathouse J S, Kirk B S, Lillard R P, et al. Crew exploration vehicle (CEV) crew module shape selection and CEV aeroscience project overview, AIAA-2007-0603[R]. Reston: AIAA, 2007.
[2] Berry S A, Horvath T J, Lillard R P, et al.Aerothermal testing for project orion crew exploration vehicle, AIAA-2009-3842[R]. Reston: AIAA, 2009.
[3] Wu Z Q, Cheng H, Zhang W, et al. Effects of thermal environment on dynamic properties of aerospace vehicle panel structures[J]. Acta Aeronautica et Astronautica Sinica, 2013, 34(2): 334-342.(in Chinese) 吴振强, 程昊, 张伟, 等. 热环境对飞行器壁板结构动特性的影响[J]. 航空学报, 2013, 34(2): 334-342.
[4] Robinson J S, Wurster K E, Mills J C. Entry trajectory and aeroheating environment definition for capsule-shaped vehicles[J]. Journal of Spacecraft and Rockets, 2009, 46(1): 74-86.
[5] Engel C D, Praharaj S C. MINIVER upgrade for the AVID system, vol. I: LANMIN user's manual[R]. NASA CR-172212, 1983.
[6] Subrahmanyam P. High-fidelity aerothermal engineering analysis for planetary probes using DOTNET framework and OLAP cubes database[J]. International Journal of Aerospace Engineering, 2009(1): 1-21.
[7] Otero R E, Braun R D. The planetary entry systems synthesis tool: a conceptual design and analysis tool for EDL systems[C]//2010 IEEE Aerospace Conference, 2010: 1-16.
[8] Park C. Stagnation-region heating environment of the Galileo probe[J]. Journal of Thermophysics and Heat Transfer, 2009, 23(3): 417-424.
[9] Anderson J D. Hypersonic and high temperature gas dynamics[M]. New York: McGraw-Hill, 1989: 156-168.
[10] Wright M, Loomis M, Padadopoulos P. Aerothermal analysis of the project fire Ⅱ afterbody flow, AIAA-2001-3065[R]. Reston: AIAA, 2001.
[11] Bertin J J. Hypersonic aerothemodynamics[M]. Washington: AIAA, 1994: 231-267.
[12] Fay J A, Riddell F R. Theory of stagnation point heat transfer in dissociated air[J]. Journal of the Aeronautical Sciences, 1958, 2(25): 73-85.
[13] Milos F S, Chen Y K. Ablation predictions for carbonaceous materials using CEA and JANNAF-based species thermodynamics[C]//42th AIAA Thermophysics Conference, 2011: 3123-3139.
[14] Potts R L. Application of integral methods to ablation charring erosion, a review[J]. Journal of Spacecraft and Rockets, 1995, 32(2): 200-209.
[15] Hu R F, Wu Z N, Qi X, et al. Debris reentry and ablation prediction and ground risk assessment software system[J]. Acta Aeronautica et Astronautica Sinica, 2011, 32(3): 390-399. (in Chinese) 胡锐锋, 吴子牛, 曲溪, 等. 空间碎片再入烧蚀预测与地面安全评估软件系统[J]. 航空学报, 2011, 32(3): 390-399.
[16] Gupta R N, Yos J M, Thompson R A, et al. A review of reaction rates and thermodynamic and transport properties for an 11-species sir model for chemical and thermal non-equilibrium calculations to 300 000 K[R]. NASA RP-1232, 1990.
[17] Park C, Lee S H. Validation of multi-temperature nozzle flow code noznt[R]. AIAA-1993-2862, 1993.
[18] Quinn R D, Gong L. Real time aerodynamic heating and surface temperature calculations for hypersonic flight simulation[R]. NASA TM-4222, 1990.
[19] Spalding D B. Convective mass transfer[M]. New York: McGraw-Hill, 1963: 156-168.
[20] Milos F S, Rassky D J. Review of numerical procedures for computational surface thermochemistry[J]. Journal of Thermophysics and Heat Transfer, 1994, 8(1): 24-34.
[21] Potts R L. On heat integral solutions of carbonaceous ablator response during re-entry, AIAA-1984-1677[R]. Reston: AIAA, 1984.
[22] Arpaci V S. Conduction heat transfer[M]. Palo Alto: Addison-Wesely, 1966: 248-257.
Outlines

/