Ionospheric D region remote sensing using VLF radio atmospherics

Lightning discharges radiate the bulk of their electromagnetic energy in the very low frequency (VLF, 3–30 kHz) and extremely low frequency (ELF, 3–3000 Hz) bands. This energy, contained in impulse-like signals called radio atmospherics or sferics, is guided for long distances by multiple reflections from the ground and lower ionosphere. This suggests that observed sferic waveforms radiated from lightning and received at long distances (>1000 km) from the source stroke contain information about the state of the ionosphere along the propagation path. The focus of this work is on the extraction of nighttime D region electron densities (in the altitude range of ∼70–95 km) from observed VLF sferics. In order to accurately interpret observed sferic characteristics, we develop a model of sferic propagation which is based on an existing frequency domain subionospheric VLF propagation code. The model shows that the spectral characteristics of VLF sferics depend primarily on the propagation path averaged ionospheric D region electron density profile, covering the range of electron densities from ∼100 to 103 cm−3. To infer the D region density from observed VLF sferics, we find the electron density profile that produces a modeled sferic spectrum that most closely matches an observed sferic spectrum. In most nighttime cases the quality of the agreement and the uncertainties involved allow the height of an exponentially varying electron density profile to be inferred with a precision of ∼0.2 km.

[1]  R. Samm,et al.  Lightning detection network averts damage and speeds restoration , 1996 .

[2]  J. A. Ferguson,et al.  Experimental Observation of Magnetic Field Effects on VLF Propagation at Night , 1970 .

[3]  David G Morfitt,et al.  'MODESRCH', An Improved Computer Program for Obtaining ELF/VLF/LF Mode Constants in an Earth-Ionosphere Waveguide , 1976 .

[4]  E. A. Mechtly,et al.  Lower ionosphere electron concentration and collision frequency from rocket measurements of Faraday rotation, differential absorption, and probe current , 1967 .

[5]  K. G. Budden The Wave-guide mode theory of wave propagation , 1963 .

[6]  E. P. Krider,et al.  The amplitude spectra of lightning radiation fields in the interval from 1 to 20 MHz , 1986 .

[7]  A.C. Fraser-Smith,et al.  The Stanford University ELF/VLF Radiometer Project: Measurement of the Global Distribution of ELF/VLF Electromagnetic Noise , 1985, 1985 IEEE International Symposium on Electromagnetic Compatibility.

[8]  James R. Wait,et al.  Characteristics of the earth-ionosphere waveguide for VLF radio waves , 1964 .

[9]  A. Farmer,et al.  The solar-terrestrial environment , 1996 .

[10]  J. Mathews,et al.  The measurement of diurnal variations of electron concentration in the 60–100 km ionosphere at Arecibo , 1982 .

[11]  A. D. Bailey,et al.  Mass spectrometric measurements of positive ions at altitudes from 64 to 112 kilometers , 1965 .

[12]  R. Barr The effect of sporadic-E on the nocturnal propagation of ELF radio waves , 1977 .

[13]  A. Gwal,et al.  Propagation of tweek atmospherics in the earth-ionosphere wave guide , 1994 .

[14]  D. Jones,et al.  An experimental investigation of ELF attenuation rates in the Earth-ionosphere duct , 1992 .

[15]  W. L. Taylor,et al.  VLF phase characteristics deduced from atmospheric wave forms , 1960 .

[16]  K. Budden The influence of the earth’s magnetic field on radio propagation by wave-guide modes , 1962, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[17]  R. Pappert,et al.  Propagation Theory and Calculations at Lower Extremely Low Frequencies (ELF) , 1974, IEEE Trans. Commun..

[18]  A. Jursa,et al.  Handbook of geophysics and the space environment , 1985 .

[19]  Neil R. Thomson,et al.  Experimental daytime VLF ionospheric parameters , 1993 .

[20]  L. Thomas,et al.  The electron density distributions in the D-region during the night and pre-sunrise period , 1970 .

[21]  Hao Ling,et al.  Wavelet analysis of radar echo from finite-size targets , 1993 .

[22]  Power spectra at radio frequency of lightning return stroke waveforms , 1989 .

[23]  Richard A. Pappert,et al.  VLF/LF mode conversion model calculations for air to air transmissions in the earth‐ionosphere waveguide , 1986 .

[24]  E. Pierce,et al.  Relations between the Character of Atmospherics and Their Place of Origin , 1957, Proceedings of the IRE.

[25]  J. Wait,et al.  Propagation Of Radio Waves , 1998, IEEE Antennas and Propagation Magazine.

[26]  E. Pierce,et al.  Leader and junction processes in the lightning discharge as a source of VLF atmospherics , 1964 .

[27]  Masashi Hayakawa,et al.  Wave characteristics of tweek atmospherics deduced from the direction-finding measurement and theoretical interpretation , 1994 .

[28]  D. G. Deeks,et al.  D-region electron distributions in middle latitudes deduced from the reflexion of long radio waves , 1966, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[29]  D. Jones,et al.  Electromagnetic radiation from multiple return strokes of lightning , 1970 .

[30]  E. T. Pierce,et al.  The return stroke of the lightning flash to earth as a source of VLF atmospherics , 1964 .

[31]  Michiko Yamashita,et al.  Propagation of tweek atmospherics , 1978 .

[32]  M. Hayakawa,et al.  One-site distance-finding technique for locating lightning discharges , 1995 .

[33]  W. L. Taylor VLF attenuation for east‐west and west‐east daytime propagation using atmospherics , 1960 .

[34]  B. Ryabov Tweek propagation peculiarities in the earth-ionosphere waveguide and low ionosphere parameters , 1992 .

[35]  B. Ryabov,et al.  Experimental investigation of the tweek field structure , 1992 .

[36]  C. Sechrist Comparisons of techniques for measurement of D‐region electron densities , 1974 .