Analysis of Radio Frequency Blackout for a Blunt-Body Capsule in Atmospheric Reentry Missions

A numerical analysis of electromagnetic waves around the atmospheric reentry demonstrator (ARD) of the European Space Agency (ESA) in an atmospheric reentry mission was conducted. During the ARD mission, which involves a 70% scaled-down configuration capsule of the Apollo command module, radio frequency blackout and strong plasma attenuation of radio waves in communications with data relay satellites and air planes were observed. The electromagnetic interference was caused by highly dense plasma derived from a strong shock wave generated in front of the capsule because of orbital speed during reentry. In this study, the physical properties of the plasma flow in the shock layer and wake region of the ESA ARD were obtained using a computational fluid dynamics technique. Then, electromagnetic waves were expressed using a frequency-dependent finite-difference time-domain method using the plasma properties. The analysis model was validated based on experimental flight data. A comparison of the measured and predicted results showed good agreement. The distribution of charged particles around the ESA ARD and the complicated behavior of electromagnetic waves, with attenuation and reflection, are clarified in detail. It is suggested that the analysis model could be an effective tool for investigating radio frequency blackout and plasma attenuation in radio wave communication.

[1]  D T Swift-Hook,et al.  Partially Ionized Gases , 1975 .

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

[3]  Chul Park,et al.  Problems of Rate Chemistry in the Flight Regimes of Aeroassisted Orbital Transfer Vehicles , 1984 .

[4]  C. F. Curtiss,et al.  Transport Properties of Multicomponent Gas Mixtures , 1949 .

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

[6]  Peter A. Gnoffo,et al.  Conservation equations and physical models for hypersonic air flows in thermal and chemical nonequilibrium , 1989 .

[7]  J. P. Appleton,et al.  The conservation equations for a non-equilibrium plasma , 1964, Journal of Fluid Mechanics.

[8]  Chul Park,et al.  Rotational Relaxation of N2 Behind a Strong Shock Wave , 2002 .

[9]  Earll M. Murman,et al.  Finite volume method for the calculation of compressible chemically reacting flows , 1985 .

[10]  Hiroshi Matsumoto,et al.  Computer experiments on radio blackout of a reentry vehicle , 2000 .

[11]  M. Sabbadini,et al.  Modelling of antenna radiation pattern of a re-entry vehicle in presence of plasma , 2004, IEEE Antennas and Propagation Society Symposium, 2004..

[12]  Francesca Vipiana,et al.  Reentry vehicles: evaluation of plasma effects on RF propagation , 2013 .

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

[14]  Yusuke Takahashi,et al.  Advanced validation of CFD-FDTD combined method using highly applicable solver for reentry blackout prediction , 2016 .

[15]  James P. Rybak,et al.  Progress in Reentry Communications , 1971, IEEE Transactions on Aerospace and Electronic Systems.

[16]  G. Mur Absorbing Boundary Conditions for the Finite-Difference Approximation of the Time-Domain Electromagnetic-Field Equations , 1981, IEEE Transactions on Electromagnetic Compatibility.

[17]  M. Fertig,et al.  TRANSPORT COEFFICIENTS FOR HIGH TEMPERATURE NONEQUILIBRIUM AIR FLOWS , 1998 .

[18]  C. Park,et al.  Assessment of two-temperature kinetic model for dissociating and weakly-ionizing nitrogen , 1986 .

[19]  J C Paulat,et al.  Re-entry Flight Experiments Lessons Learned - The Atmospheric Reentry Demonstrator ARD , 2007 .

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

[21]  I. F. Belov,et al.  Investigation of Remote Antenna Assembly for Radio Communication with Reentry Vehicle , 2001 .

[22]  Michael Keidar,et al.  Analysis of an Electromagnetic Mitigation Scheme for Reentry Telemetry Through Plasma , 2008 .

[23]  Takashi Abe,et al.  Examination of Radio Frequency Blackout for an Inflatable Vehicle During Atmospheric Reentry , 2014 .

[24]  Antony Jameson,et al.  Lower-upper implicit schemes with multiple grids for the Euler equations , 1987 .

[25]  Eric Michielssen,et al.  A FMM-FFT accelerated hybrid volume surface integral equation solver for electromagnetic analysis of re-entry space vehicles , 2014, 2014 USNC-URSI Radio Science Meeting (Joint with AP-S Symposium).

[26]  Bernd Einfeld On Godunov-type methods for gas dynamics , 1988 .

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

[28]  C. F. Curtiss,et al.  Molecular Theory Of Gases And Liquids , 1954 .

[29]  S.,et al.  Numerical Solution of Initial Boundary Value Problems Involving Maxwell’s Equations in Isotropic Media , 1966 .

[30]  J. Yos,et al.  TRANSPORT PROPERTIES OF NITROGEN, HYDROGEN, OXYGEN, AND AIR TO 30,000 K , 1963 .

[31]  Takashi Abe,et al.  Frequency-Dependent FDTD Simulation of the Interaction of Microwaves With Rocket-Plume , 2010, IEEE Transactions on Antennas and Propagation.

[32]  Takashi Abe,et al.  Prediction Performance of Blackout and Plasma Attenuation in Atmospheric Reentry Demonstrator Mission , 2014 .

[33]  M.D. White Simulation of communications through a weakly ionized plasma for a re-entry vehicle at Mach 23.9 , 2005, 2005 IEEE Antennas and Propagation Society International Symposium.

[34]  S. L. Petrie,et al.  Free electron and vibrational temperature nonequilibrium in high temperature nitrogen , 1974 .

[35]  K. Singh,et al.  Transport properties of multicomponent gas mixtures and status of intermolecular potential , 1990 .

[36]  Michio Nishida,et al.  Thermochemical Nonequilibrium in Rapidly Expanding Flows of High-Temperature Air , 1997 .

[37]  Jong-Hun Lee Electron-impact vibrational relaxation in high-temperature nitrogen , 1992 .