2007
DOI: 10.1109/temc.2007.902179
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Generalized Form of Telegrapher's Equations for the Electromagnetic Field Coupling to Finite-Length Lines Above a Lossy Ground

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Cited by 40 publications
(18 citation statements)
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“…The fundamental parameter to understanding the behaviour of induced fields is the knowledge of the current distribution induced on the line. This induced current generates scattered fields that not only propagate away from the equipment but also generate the so-called scattered voltage along the line [4]. Two models for the analysis of electromagnetic field coupling to finite length lines based on the wire antenna theory and transmission line model, respectively, in the frequency and time domain are outlined in this section.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
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“…The fundamental parameter to understanding the behaviour of induced fields is the knowledge of the current distribution induced on the line. This induced current generates scattered fields that not only propagate away from the equipment but also generate the so-called scattered voltage along the line [4]. Two models for the analysis of electromagnetic field coupling to finite length lines based on the wire antenna theory and transmission line model, respectively, in the frequency and time domain are outlined in this section.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…The spatial current distribution along the overhead wire, shown in Fig 1, is governed by the Pocklington integro-differential equation [4]:…”
Section: The Antenna Model: Frequency and Time Domain Analysismentioning
confidence: 99%
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“…However, most of the studies related to the thin wire radiating in the presence of a twomedia configuration are usually carried out in the frequency domain [1][2][3][4][5][6][7][8][9][10][11][12]. The corresponding time domain parameters then can be obtained using the inverse Fourier transform.…”
Section: Introductionmentioning
confidence: 99%