Formulations via scalar potentials
As we have already remarked in the preceding chapters, a specific feature of eddy current problems is the presence of differential constraints acting in the non-conducting part of the domain: namely, curl H I =J e,I in Ω I and div (ε I E I )=0 in Ω I
KeywordsNumerical Approximation Weak Formulation Scalar Potential Element Approximation Edge Element
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