2006
DOI: 10.1049/ip-map:20045113
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Innovative basis and weight functions for wire junctions in time domain moment method

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Cited by 6 publications
(17 citation statements)
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“…A generic scattering body S may contain a planar part S T to be subdivided into a mesh-grid of planar patches and a wire part S W to be subdivided into a mesh-grid of piece-wise rectilinear segments of radius a as shown in S T a Rao-Wilton-Glisson (RWG) spatial basis is defined along the two triangular patches sharing it [10,16] and for each non boundary node in S W a wire basis function is defined on the two wire segments sharing it [1,9]. The attachment comprises one or more triangular patches, sharing a vertex node, and one segment connected to that same node.…”
Section: Theorymentioning
confidence: 99%
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“…A generic scattering body S may contain a planar part S T to be subdivided into a mesh-grid of planar patches and a wire part S W to be subdivided into a mesh-grid of piece-wise rectilinear segments of radius a as shown in S T a Rao-Wilton-Glisson (RWG) spatial basis is defined along the two triangular patches sharing it [10,16] and for each non boundary node in S W a wire basis function is defined on the two wire segments sharing it [1,9]. The attachment comprises one or more triangular patches, sharing a vertex node, and one segment connected to that same node.…”
Section: Theorymentioning
confidence: 99%
“…The time basis T h (t) is usually selected as a C 0 (continuous) or more regular (C 1 , continuous and differentiable) function whose value is 1 for t = 0 and zero for t = n∆t for non-zero integer values of n. The choice of these interpolation functions is far from being trivial because it deeply affects both accuracy and stability, as analyzed in [9].…”
Section: Theorymentioning
confidence: 99%
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