2020 IEEE Power &Amp; Energy Society General Meeting (PESGM) 2020
DOI: 10.1109/pesgm41954.2020.9281776
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Study of Skin and Proximity Effects of Conductors for MTL-Based Modeling of Power Transformers Using FEM

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Cited by 3 publications
(6 citation statements)
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“…Hence, it covers the edges very well. The magnetic vector potential A(x, y) = A z (x, y) ẑ and, consequently, the current density distribution is calculated by solving the diffusion equation [29] ∇ 2 A z (x, y)−jωσ(x, y)µ(x, y)A z (x, y)+µ(x, y)J ez (x, y) = 0. ( 16)…”
Section: Skin Effectmentioning
confidence: 99%
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“…Hence, it covers the edges very well. The magnetic vector potential A(x, y) = A z (x, y) ẑ and, consequently, the current density distribution is calculated by solving the diffusion equation [29] ∇ 2 A z (x, y)−jωσ(x, y)µ(x, y)A z (x, y)+µ(x, y)J ez (x, y) = 0. ( 16)…”
Section: Skin Effectmentioning
confidence: 99%
“…A z (x, y) goes to zero at infinity. To solve (16), the Dirichlet boundary condition (i.e., A z (x, y) = 0) at a far enough boundary is employed (i.e., truncating the outer boundary at a distance much larger than a conductor size) [20,29,44]. In this section, ( 16) is solved at each frequency using the PGD approach and approximated as…”
Section: Skin Effectmentioning
confidence: 99%
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