1972
DOI: 10.1109/tct.1972.1083513
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Transient analysis of coaxial cables using the skin effect approximationA+Bsqrt{s}

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Cited by 118 publications
(36 citation statements)
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“…In general, the impedance is a nonlinear function of frequency. Thus, the description of the frequency dependent loss is introduced by using the widely used Nahman approximation of the internal impedance Z int (s) = A + B √ s as in [12] and Qingjian formulation of conductance [13], where s is the Laplace transform variable.…”
Section: Analysis Of Nmtl Using the Fdtd Methodsmentioning
confidence: 99%
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“…In general, the impedance is a nonlinear function of frequency. Thus, the description of the frequency dependent loss is introduced by using the widely used Nahman approximation of the internal impedance Z int (s) = A + B √ s as in [12] and Qingjian formulation of conductance [13], where s is the Laplace transform variable.…”
Section: Analysis Of Nmtl Using the Fdtd Methodsmentioning
confidence: 99%
“…In time domain and according to the expression of Z int in [12], the convolution product Z int (z, t) * I (z, t) becomes:…”
Section: Analysis Of Nmtl Using the Fdtd Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Other skin effect models for lower frequencies are the cylindrical skin effect [27] and the f m -law with 0 < m < 1 as described in [26]. The general case including dielectric losses is discussed in [28] and [26], and a model considering a non-zero dc resistance of the inner conductor is presented in [29]. However, the aforementioned models cannot be represented by closed form analytic expressions.…”
Section: B Short-circuited Infinitely Long Cablementioning
confidence: 99%
“…La impedancia interna de conductores cilíndricos para grandes parámetros puede ser calculada mediante ciertos modelos aproximados, los cuales no involucran el cálculo de las funciones de Bessel, funciones de Bessel modificadas o funciones de Kelvin y por lo tanto permiten determinar la impedancia interna de una manera más sencilla con poco esfuerzo computacional. Sin embargo, estos modelos no son exactos y presentan cierto margen de error, por lo que son clasificados como modelos de baja precisión, tales como los propuestos por Nahman y Holt [9], Semlyen y Deri [10], Wedepohl y Wilcox [11]; y modelos de alta precisión, como los propuestos por Vujević, Boras y Sarajčev [12], Mingli y Yu [13], Knight [14].…”
Section: Introductionunclassified