FDTD Analysis of Electric Fields at Ground Level Generated by Compact Intracloud Discharges

Using the finite-difference time-domain (FDTD) method for solving Maxwell's equations, we have studied waveguiding properties of a large low-conductivity cylinder, having a length of about 1000 m, a radius of 100 m, permittivity equal to the vacuum permittivity, permeability equal to vacuum permeability, and a conductivity of 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup> to <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$10^{-5} \mathrm{S} / \mathrm{m}$</tex>. The cylinder simulates a compact intracloud discharge (CID). It is placed at altitudes from 14 to 21 km above ground, excited by a voltage source at the center, and the resultant vertical electric fields on the ground surface at horizontal distances from 14 to 38 km from the cylinder are computed. The FDTD-computed vertical electric field waveforms roughly match the corresponding measured ones for the excitation voltage pulse with a half-peak width of 30 microseconds, but not for the 5 microsecond ramp followed by a constant value. The results indicate that the CID representation by a large lowconductivity cylinder is reasonable.

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Publication Details

Published
2025-06-17
DOI
https://doi.org/10.1109/apl65034.2025.11108748
Citations
1
Primary Topic
Plasma Diagnostics and Applications
Type
article
Field-Weighted Citation Impact
0.73
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article

FDTD Analysis of Electric Fields at Ground Level Generated by Compact Intracloud Discharges

Yoshihiro Baba, Vladimir A. Rakov, Shota Ueda
1 citations
Plasma Diagnostics and Applications
0.73
article

FDTD Analysis of Electric Fields at Ground Level Generated by Compact Intracloud Discharges

Yoshihiro Baba, Vladimir A. Rakov, Shota Ueda
article en
1 citations

Abstract

Using the finite-difference time-domain (FDTD) method for solving Maxwell's equations, we have studied waveguiding properties of a large low-conductivity cylinder, having a length of about 1000 m, a radius of 100 m, permittivity equal to the vacuum permittivity, permeability equal to vacuum permeability, and a conductivity of 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup> to <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$10^{-5} \mathrm{S} / \mathrm{m}$</tex>. The cylinder simulates a compact intracloud discharge (CID). It is placed at altitudes from 14 to 21 km above ground, excited by a voltage source at the center, and the resultant vertical electric fields on the ground surface at horizontal distances from 14 to 38 km from the cylinder are computed. The FDTD-computed vertical electric field waveforms roughly match the corresponding measured ones for the excitation voltage pulse with a half-peak width of 30 microseconds, but not for the 5 microsecond ramp followed by a constant value. The results indicate that the CID representation by a large lowconductivity cylinder is reasonable.

Doshisha University (JP), University of Florida (US)
Openalex Percentile: Top 25%
Plasma Diagnostics and Applications
0.73
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