2013
DOI: 10.2528/pierm13042405
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On the Success of Electromagnetic Analytical Approaches to Full Time-Domain Formulation of Skin Effect Phenomena

Abstract: Abstract-Maxwell equations can be used to formulate an analytical full time-domain theory of skin effect phenomena in circular cylindrical conductors without any detour into the frequency domain. The paper shows how this can be done and concomitantly provides the means to determine the time-varying per unit length voltage drop along the conductor from a given time-varying conductor current. The developed relationship between voltage and current is not very complicated and led the authors to examine the reasons… Show more

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Cited by 7 publications
(9 citation statements)
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“…However, even though this transient approach gives the correct results at low frequencies and is consistent with Bessel function solutions it turns out that the series solution diverges if the ratio conductor radius to skin depth a/δ exceeds 2.7. This coincidentally is close to the mathematical irrational number e=2.718... [1,8]. This divergence has been considered previously to be a consequence of mathematical inversion but this has not yet been proved for the power series case.…”
Section: Introductionsupporting
confidence: 64%
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“…However, even though this transient approach gives the correct results at low frequencies and is consistent with Bessel function solutions it turns out that the series solution diverges if the ratio conductor radius to skin depth a/δ exceeds 2.7. This coincidentally is close to the mathematical irrational number e=2.718... [1,8]. This divergence has been considered previously to be a consequence of mathematical inversion but this has not yet been proved for the power series case.…”
Section: Introductionsupporting
confidence: 64%
“…Hence, where S, T o , T 1 ... etc are functions of time. After differentiating equation (6) and after some considerable algebra [9] which involves inversion of the power series for the current ('brute force approach', [12]) or using matrix inversion algebra [1,10] the emf becomes where μ=μ o μ r /(4π) and I ( m) is the mth derivative of the current. I is the current, R o and L o are the low frequency resistance and inductance respectively.…”
Section: Vector Potential Methodsmentioning
confidence: 99%
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“…Note 2: In the case of imperfect wires, the result in (17) must be modified to include perturbation terms due to skin effect. Time‐domain skin effect terms require i ( t ) and all its time‐derivatives to be known .…”
Section: Maxwell's Equationsmentioning
confidence: 99%