Analysis of weakly ionized ablation plasma flows for a hypersonic vehicle

Abstract Hypersonic vehicles are enveloped by a plasma sheath that affects the data transmission and object identification. This paper develops a numerical methodology based on Magnetohydrodynamics equations to study the electromagnetic environment of hypersonic vehicles under the condition of carbon-based thermal protection material ablation. A surface ablation model considering the oxidation and sublimation ablation process is coupled with a Navier–Stokes solver by a gas–solid interaction method to simulate the ablation plasma flows. A piecewise linear current density recursive convolution finite-difference time-domain method is applied to further analyze the interaction between the incident electromagnetic wave and the plasma sheath. The computational results for an HTV-2 type vehicle indicate that both ablation and non-ablation plasma sheaths have significant effects on the electromagnetic environment of the vehicle. Compared with a non-ablation plasma sheath, ablation results in a decrease in the number of electrons and increases the number of neutral particles and therefore changes characteristic parameters of the plasma. Details of the electromagnetic scattering characteristics are reported to highlight the influences of ablation on the reflectivity, penetrability, and absorptivity of the plasma sheath for incident electromagnetic waves over different bands.

[1]  Shaobin Liu,et al.  A novel FDTD formulation for dispersive media , 2003 .

[2]  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 .

[3]  J. G. Parker Rotational and Vibrational Relaxation in Diatomic Gases , 1959 .

[4]  L. K. Sproul,et al.  Influence of reentry turbulent plasma fluctuation on EM wave propagation , 2006 .

[5]  Paul Lewis,et al.  Radio Frequency (RF) Blackout During Hypersonic Reentry , 2005 .

[6]  F. Blottner,et al.  Chemically Reacting Viscous Flow Program for Multi-Component Gas Mixtures. , 1971 .

[7]  K. Kunz,et al.  Finite-difference time-domain analysis of gyrotropic media. I. Magnetized plasma , 1992 .

[8]  D. Giordano Hypersonic-Flow Governing Equations with Electromagnetic Files , 2002 .

[9]  Chul Park,et al.  STAGNATION-POINT HEAT TRANSFER RATES FOR PIONEER-VENUS PROBES , 1999 .

[10]  Roger C. Millikan,et al.  Systematics of Vibrational Relaxation , 1963 .

[11]  F. Blottner Prediction of electron density in the boundary layer on entry vehicles with ablation , 1970 .

[12]  Harry Partridge,et al.  Chemical-kinetic parameters of hyperbolic Earth entry , 2000 .

[13]  Konstantinos T. Panourgias,et al.  A fully implicit scheme for simulating ionized gas flows using the gas dynamics electrodynamics coupled system , 2014 .

[14]  R. Luebbers,et al.  The Finite Difference Time Domain Method for Electromagnetics , 1993 .

[15]  Michael Keidar,et al.  Electromagnetic Reduction of Plasma Density During Atmospheric Reentry and Hypersonic Flights , 2008 .

[16]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[17]  S. V. Zhluktov,et al.  Viscous Shock-Layer Simulation of Airflow past Ablating Blunt Body with Carbon Surface , 1999 .

[18]  Steven Walker,et al.  The DARPA/AF Falcon Program: The Hypersonic Technology Vehicle #2 (HTV-2) Flight Demonstration Phase , 2008 .

[19]  D. Bianchi,et al.  Aerothermodynamic analysis of reentry flows with coupled ablation , 2011 .

[20]  Bruce Archambeault,et al.  The Finite-Difference Time-Domain Method , 1998 .

[21]  Alireza Mazaheri,et al.  A Study of Ablation-Flowfield Coupling Relevant to the Orion Heatshield , 2012 .

[22]  Qiang Chen,et al.  An FDTD formulation for dispersive media using a current density , 1998 .

[23]  Donald L. Potter Introduction of the PIRATE Program for Parametric Reentry Vehicle Plasma Effects Studies , 2006 .

[24]  Emanuele Martelli,et al.  Navier-Stokes Simulations of Hypersonic Flows with Coupled Graphite Ablation , 2010 .

[25]  Chul Park,et al.  Assessment of two-temperature kinetic model for ionizing air , 1987 .

[26]  Frank S. Milos,et al.  Navier-Stokes Solutions with Finite Rate Ablation for Planetary Mission Earth Reentries , 2005 .

[27]  Joe LoVetri,et al.  A comparison of numerical techniques for modeling electromagnetic dispersive media , 1995 .

[28]  A. Jameson,et al.  Lower-upper Symmetric-Gauss-Seidel method for the Euler and Navier-Stokes equations , 1988 .

[29]  Xiang He,et al.  Numerical calculation on electromagnetic wave reflection by plasma-covered structures , 2012, ISAPE2012.

[30]  L. Eriksson Generation of boundary-conforming grids around wing-body configurations using transfinite interpolation , 1982 .

[31]  Dinesh K. Prabhu,et al.  Current Grid Generation Strategies and Future Requirements in Hypersonic Vehicle Design, Analysis and Testing , 1999 .

[32]  William F. Bailey,et al.  Governing Equations for Weakly Ionized Plasma Flowfields of Aerospace Vehicles , 2002 .

[33]  D. R. Stull JANAF thermochemical tables , 1966 .

[34]  Oh-Hyun Rho,et al.  Methods for the accurate computations of hypersonic flows: I. AUSMPW + scheme , 2001 .

[35]  X. Kong,et al.  Calculation of the Effect on the Reflection of the Plane Electromagnetic Wave for Non-Magnetized Plasma with Different Electron Density Distributions , 2007 .

[36]  R. J. Luebbers,et al.  Piecewise linear recursive convolution for dispersive media using FDTD , 1996 .