Features of Afterbody Radiative Heating for Earth Entry

Radiative heating is identified as a major contributor to afterbody heating for Earth entry capsules at velocities above 10  km/s. Because of rate-limited electron–ion recombination processes, many of the electronically excited N and O atoms produced in the high-temperature/pressure forebody remain as they expand into the afterbody region, which results in significant afterbody radiation. Large radiative heating sensitivities to electron-impact ionization rates and escape factors are identified. Ablation products from a forebody ablator are shown to increase the afterbody radiation by nearly 40%, due to the influence of CO on the vibrational-electronic temperature. The tangent-slab radiation transport approach is shown to overpredict the radiative flux by as much as 50% in the afterbody, therefore making the more computationally expensive ray-tracing approach necessary for accurate radiative flux predictions. For the Stardust entry, the afterbody radiation is predicted to be nearly twice as large as the c...

[1]  Determination of the emissivity of materials , 1962 .

[2]  W. D. Goodrich,et al.  The aerothermodynamic environment of the Apollo command module during superorbital entry , 1972 .

[3]  Chul Park Comparison of electron and electronic temperatures in recombining nozzle flow of ionized nitrogen—hydrogen mixture. Part 1. Theory , 1973, Journal of Plasma Physics.

[4]  C. Park,et al.  Nonequilibrium Hypersonic Aerothermodynamics , 1989 .

[5]  Richard A. Thompson,et al.  A review of reaction rates and thermodynamic and transport properties for the 11-species air model for chemical and thermal nonequilibrium calculations to 30000 K , 1989 .

[6]  Charles H. Kruger,et al.  Ionization nonequilibrium induced by neutral chemistry in air plasmas , 1996 .

[7]  Wolfgang L. Wiese,et al.  Atomic Transition Probabilities of Carbon, Nitrogen, and Oxygen: A Critical Data Compilation , 1996 .

[8]  Bourdon,et al.  Three-body recombination rate of atomic nitrogen in low-pressure plasma flows. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[9]  W. Willcockson Stardust Sample Return Capsule Design Experience , 1998 .

[10]  Mark Loomis,et al.  Aerothermal analysis of the Project Fire II afterbody flow , 2001 .

[11]  Sanford Gordon,et al.  NASA Glenn Coefficients for Calculating Thermodynamic Properties of Individual Species , 2002 .

[12]  Takashi Abe,et al.  Assessment of Forebody and Backbody Radiative Heating Rate of Hypervelocity Reentry Capsule , 2003 .

[13]  Chul Park,et al.  Effect of Lymann Radiation on Nonequilibrium Ionization of Atomic Hydrogen , 2004 .

[14]  Michael J. Wright,et al.  Afterbody Aeroheating Flight Data for Planetary Probe Thermal Protection System Design , 2006 .

[15]  Christopher O. Johnston,et al.  Non-Boltzmann Modeling for Air Shock-Layer Radiation at Lunar-Return Conditions , 2008 .

[16]  Dinesh K. Prabhu,et al.  Radiation Modeling for the Reentry of the Stardust Sample Return Capsule , 2008 .

[17]  B. Hollis,et al.  Spectrum Modeling for Air Shock-Layer Radiation at Lunar-Return Conditions , 2008 .

[18]  Chul B. Park The Limits of Two-Temperature Kinetic Model in Air , 2010 .

[19]  Alireza Mazaheri,et al.  LAURA Users Manual: 5.3-48528 , 2010 .

[20]  Peter Jenniskens,et al.  Observations of the Stardust Sample Return Capsule Entry with a Slitless Echelle Spectrograph , 2010 .

[21]  S. Surzhikov,et al.  Simulating Stardust Earth Reentry with Radiation Heat Transfer , 2011 .

[22]  Christopher O. Johnston,et al.  Shock Layer Radiation Modeling and Uncertainty for Mars Entry , 2012 .

[23]  L. Marraffa,et al.  Aerothermal analysis of the Phoebus capsule with radiative heating on the back body , 2012 .

[24]  P. Omaly,et al.  Global rate coefficients for ionization and recombination of carbon, nitrogen, oxygen, and argon , 2012 .

[26]  Christopher O. Johnston,et al.  Uncertainty Analysis of Air Radiation for Lunar-Return Shock Layers , 2012 .

[27]  Marco Panesi,et al.  QCT-based vibrational collisional models applied to nonequilibrium nozzle flows , 2012 .

[28]  Alireza Mazaheri,et al.  Radiative Heating Uncertainty for Hyperbolic Earth Entry, Part 1: Flight Simulation Modeling and Uncertainty , 2013 .

[29]  Andrea Lani,et al.  Collisional radiative coarse-grain model for ionization in air , 2013 .

[30]  Andrea Lani,et al.  Modeling of non-equilibrium phenomena in expanding flows by means of a collisional-radiative model , 2013 .

[31]  A. Bourdon,et al.  Consistent multi-internal-temperatures models for nonequilibrium nozzle flows , 2013 .

[32]  C. Johnston,et al.  Three-Dimensional Radiation Ray-Tracing for Shock-Layer Radiative Heating Simulations , 2013 .