2013
DOI: 10.1007/978-1-4419-8429-6
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Computational Electromagnetics and Model-Based Inversion

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Cited by 34 publications
(16 citation statements)
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“…In our model-based inverse problems, the impedance Z = g(p 1 , · · · , p N , f ) which depends on N unknown parameters p N (such as length, width, depth) and a control parameter f (such as frequency, scan-position, lift-off) [3]. In order to determine p 1 …”
Section: Methodsmentioning
confidence: 99%
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“…In our model-based inverse problems, the impedance Z = g(p 1 , · · · , p N , f ) which depends on N unknown parameters p N (such as length, width, depth) and a control parameter f (such as frequency, scan-position, lift-off) [3]. In order to determine p 1 …”
Section: Methodsmentioning
confidence: 99%
“…The problem consists of a split-D probe of the type shown in Fig. 1, and which was analyzed in [3] that is scanned past a rectangular slot whose dimensions are 1mm×2mm×3mm. The probe is vertical to the surface of the workpiece, but is rotated about its axis by 22…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…In our model-based inverse problems, the impedance Z = g(p 1 , · · · , p N , f ) which depends on N unknown parameters p N (such as length, width, depth) and a control parameter f (such as frequency, scan-position, lift-off) [3]. In order to determine p 1 , · · · , p N , we measure Z at M frequencies f 1 , · · · , f M ,…”
Section: Methodsmentioning
confidence: 99%
“…With this method, a powerful interpolation can be made with fewer support nodes than that on a full grid. In this work, we combined the sparse grid toolbox, TASMANIAN [2], which is produced by Oak Ridge National Laboratory, and professional eddy-current NDE software VIC-3D R [3] to solve a specific inverse problem. In this problem, a crack was simulated by four blocks which each of them having a different depth.…”
Section: Introductionmentioning
confidence: 99%