2014
DOI: 10.1080/17415977.2014.969728
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Simultaneous numerical determination of a corroded boundary and its admittance

Abstract: Abstract. In this paper, an inverse geometric problem for Laplace's equation arising in boundary corrosion detection is considered. This problem, which consists of determining an unknown corroded portion of the boundary of a bounded domain and its admittance Robin coefficient from two pairs of boundary Cauchy data (boundary temperature and heat flux), is solved numerically using the meshless method of fundamental solutions. A nonlinear minimisation of the objective function is regularised, and the stability of… Show more

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Cited by 4 publications
(5 citation statements)
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References 30 publications
(26 reference statements)
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“…where ν is the outward unit normal to ∂D and 0 < λ ∈ C(∂D) or L ∞ (∂D) is a Robin coupling real function usually called the impedance function, [15], or admittance, [8]. When λ → 0 or λ → ∞ we obtain the particular cases of a sound-hard or sound-soft scatterer, respectively.…”
Section: Mathematical Formulationmentioning
confidence: 99%
“…where ν is the outward unit normal to ∂D and 0 < λ ∈ C(∂D) or L ∞ (∂D) is a Robin coupling real function usually called the impedance function, [15], or admittance, [8]. When λ → 0 or λ → ∞ we obtain the particular cases of a sound-hard or sound-soft scatterer, respectively.…”
Section: Mathematical Formulationmentioning
confidence: 99%
“…There is a considerable amount of literature available, dealing with both theoretical and computational aspects of both the individual problems, i.e. estimation of the Robin coefficient or estimation of the domain shape, see e.g [1][2][3][5][6][7][8][9][10][11][12][13][14][15], as well as of the problem of joint estimation [16][17][18][19][20][21][22][23][24][25][26]. We also mention the works [27,28], in which a similar problem is considered using a generalized impedance boundary condition.…”
Section: Introductionmentioning
confidence: 99%
“…When D is a rigid inclusion ( ) λ = ∞ or a cavity ( ) λ = 0 ; see, e.g. [27] for the physical explanation, we can formulate the initialboundary value problem and define the Neumann-to-Dirichlet map analogously. The inverse problem for active thermography is to reconstruct D from the measured data Λ D .…”
Section: Introductionmentioning
confidence: 99%
“…In [19,20], the inverse problem is form ulated as a shape optimization problem and is solved by optimization methods. A meshless method of fundamental solutions is proposed in [12], where | = u t 0 is nonzero and D can depend on t. This method is also applied to simultaneously reconstruct D and λ for the Laplace equation case; see [27]. As for non-iterative reconstruction methods, we refer to [10,11,23,25,26,29,39] and the references therein, where the dynamical probe method and the enclosure method are developed.…”
Section: Introductionmentioning
confidence: 99%