2013
DOI: 10.1002/mma.2947
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Corner asymptotics of the magnetic potential in the eddy‐current model

Abstract: Abstract:In this paper, we describe the scalar magnetic potential in the vicinity of a corner of a conducting body embedded in a dielectric medium in a bidimensional setting. We make explicit the corner asymptotic expansion for this potential as the distance to the corner goes to zero. This expansion involves singular functions and singular coefficients. We introduce a method for the calculation of the singular functions near the corner and we provide two methods to compute the singular coefficients: the metho… Show more

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Cited by 8 publications
(9 citation statements)
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References 15 publications
(52 reference statements)
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“…However, there is no improvement for the H 1 ‐norm, which remains scriptOfalse(εfalse). We present here a method of profile correction similar to other studies . The idea consists in precomputing the profiles frakturK and frakturz, and to build the correction v˜ε(x)=vε(x)+γε(Kz)boldxε, which gives a better approximation of unormaliε in the H 1 ‐norm.…”
Section: Profile Correctionmentioning
confidence: 99%
See 1 more Smart Citation
“…However, there is no improvement for the H 1 ‐norm, which remains scriptOfalse(εfalse). We present here a method of profile correction similar to other studies . The idea consists in precomputing the profiles frakturK and frakturz, and to build the correction v˜ε(x)=vε(x)+γε(Kz)boldxε, which gives a better approximation of unormaliε in the H 1 ‐norm.…”
Section: Profile Correctionmentioning
confidence: 99%
“…We present here a method of profile correction similar to other studies. [53][54][55] The idea consists in precomputing the profiles and , and to build the correctionṽ…”
Section: Profile Correctionmentioning
confidence: 99%
“…A first idea consists in correcting the approximate solution v ε with the difference γ √ ε(K − Z) x ε , the profiles Z and K being computed as a preliminary step. This kind of method has been introduced in [14,24,26] for similar problems, see also a remark in [27,Appendix B.5.2]. Here are the steps of the algorithm…”
Section: Correction With Transmission Profilesmentioning
confidence: 99%
“…Let K(αj) be the part of the dual solution associated with the negative eigenvalue α j , so that K(ρ,ϕ,z)=jK(αj)(ρ,ϕ,z)1emand1emK(αj)(ρ,ϕ,z)==0,2,4,6zBk(z)ραk+ψk,(ρ,ϕ) Following the construction of dual singularities introduced in , it appears here that the dual singularities K(αj), which are associated with an integer eigenvalue αjdouble-struckZ, contain logarithmic terms in ρ . In this paper, we make the following ansatz for these dual singularities: K(αj)(ρ,ϕ,z)==0,2,4,6zBj(z)ραj+()ψj,(ϕ)+logρ0.3emtrueψ~j,(ϕ), and hereafter, we provide explicit recursive ODEs for the determination of the corresponding polar parts ψ j , ℓ ( ϕ )and trueψ~j,(ϕ).…”
Section: Dual Solution With Logarithmic Terms Associated With Integermentioning
confidence: 99%
“…For homogeneous Neumann BCs, we have first to consider α 0 =0. For α 0 =0, there is no dual eigenvalue, so we use the logarithmic solution presented in to obtain K(α0=0): K(α0=0)=B0(z)logρ+B0′′(z)ρ214(1logρ)+B0(4)(z)ρ43128+logρ164+B0(6)(z)ρ61113824logρ12304+ The next integer dual eigenvalue is α 2 =−1, and for it, K(α2=1) is K(α2=1)=ρ1B2(z)cosϕB2′′(z)ρ2logρcosϕ2+B2(4)(z)ρ4364+logρ116cosϕ<...>…”
Section: Dual Solution With Logarithmic Terms Associated With Integermentioning
confidence: 99%