2008
DOI: 10.2528/pierl07112904
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An Analytic Formula of the Current Distribution for the VLF Horizontal Wire Antenna Above Lossy Half-Space

Abstract: Abstract-An analytical formula of the current distribution for the VLF horizontal wire antenna located above the ground is presented in this paper. This formula is suitable for the VLF horizontal antenna which is fed at arbitrary position and with arbitrary loaded impedance at the end. In order to validate the analytical formula, a numerical code based on MoM is also developed. The comparison between the results obtained by two methods proves the validity of the analytical formula proposed in this paper.

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Cited by 12 publications
(6 citation statements)
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“…Theoretically, the dipole antenna is a resonance structure and supports a standing wave of current. However, the current distribution can be altered to support a traveling wave with attenuation while traveling from the feed point to the terminations of the dipole arms [23,24]. This is true for photoconductive antennas possessing very long DC bias striplines with open-circuited terminations in a high dielectric constant substrate, because there is little current to be reflected back owing to the radiation as the current travels along the long striplines.…”
Section: Introductionmentioning
confidence: 99%
“…Theoretically, the dipole antenna is a resonance structure and supports a standing wave of current. However, the current distribution can be altered to support a traveling wave with attenuation while traveling from the feed point to the terminations of the dipole arms [23,24]. This is true for photoconductive antennas possessing very long DC bias striplines with open-circuited terminations in a high dielectric constant substrate, because there is little current to be reflected back owing to the radiation as the current travels along the long striplines.…”
Section: Introductionmentioning
confidence: 99%
“…The problem of calculating the radiated fields from a horizontal electric dipole antenna over a halfspace is a classical problem in electromagnetics and is often the starting point for many simulations of Ground Penetrating Radar (GPR). It has been extensively studied, beginning with Sommerfeld in 1909 [26,27], with further work by [1,13,29], and more recently [2,4,8,16,17,21,22]. The aim of this research is to compare solutions to this problem using current implementations of the most commonly used numerical techniques, namely: the Finite-Difference Time-Domain (FDTD) method; the Finite-Integration Technique (FIT); and Time-Domain Integral Equation (TDIE) methods.…”
Section: Introductionmentioning
confidence: 99%
“…The variety of available vibrator structures and also creation of new constructions on their basis stipulate constant interest of investigators to the problems of their analysis and synthesis. So, for example, location of different active and passive elements in definite points along the length of a vibrator's antenna and also vibrator's excitation in a distinctive from its centre point create additional opportunities to form the set electrodynamic characteristics of vibrator radiators [1][2][3][4][5]. From our point of view, thin vibrators, on the surface of which impedance boundary conditions are performed, can serve these aims [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21].…”
Section: Introductionmentioning
confidence: 99%