1979
DOI: 10.1109/tmag.1979.1070317
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Computational methods for solving static field and eddy current problems via Fredholm integral equations

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Cited by 48 publications
(6 citation statements)
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“…where j j is the potential of the jth part of the system (Harrington, 1968(Harrington, /1993McWhirter et al, 1979;Chari and Salon, 2000). After obtaining the distributions of vectors B (B ¼ curl A) and E of the electromagnetic field in the investigated area, we can also determine the distribution of the Poynting vector N using the expression:…”
Section: Mathematical Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…where j j is the potential of the jth part of the system (Harrington, 1968(Harrington, /1993McWhirter et al, 1979;Chari and Salon, 2000). After obtaining the distributions of vectors B (B ¼ curl A) and E of the electromagnetic field in the investigated area, we can also determine the distribution of the Poynting vector N using the expression:…”
Section: Mathematical Modelmentioning
confidence: 99%
“…where j j is the potential of the jth part of the system (Harrington, 1968(Harrington, /1993McWhirter et al, 1979;Chari and Salon, 2000).…”
Section: Mathematical Modelmentioning
confidence: 99%
“…McWhirter [69] developed computational methods for solving 2D quasi-static problems by solving the Fredholm equation of the second kind. Lean [70][71][72] used the BEM to solve eddy current problems in 2D, and gave a good overview of boundary integral methods in electromagnetics [73].…”
Section: Boundary Elementsmentioning
confidence: 99%
“…103 More complex two-and three-dimensional basis functions have been used in magnet design. 80 While this approach has to be carefully monitored in initial-value MHD problems due to the need to repeat the calculation many times, it can be more efficient to use higher-order basis functions. Each of these techniques is a special case of the weighted Galerkin finite element method.…”
Section: Spatial and Temporal Discretisationmentioning
confidence: 99%