Abstract
Since the line loop current is equivalent to the double layer charge, it gives an integral form of scalar potential. The segmental loop current on the interface between magnetic materials produces a potential gap, which works to give a boundary integral equation (BIE). By virtue of another potential gap due to a fictitious circulating current along the contour of cut-surface in the material, the excitation potential becomes single valued and the BIE becomes applicable to generic problems without any restriction. Regarding the nonlinear magnetic material as composed of segmental materials with different values of permeability, we get the same BIE for the nonlinear analysis as for the linear analysis. In order to check the adequacy and effectiveness of the nonlinear BIE, we solve a typical magnetostatic problem and compare the computed results with those by the conventional magnetic moment method.
Original language | English |
---|---|
Article number | 6514577 |
Pages (from-to) | 1573-1576 |
Number of pages | 4 |
Journal | IEEE Transactions on Magnetics |
Volume | 49 |
Issue number | 5 |
DOIs | |
Publication status | Published - 2013 |
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Keywords
- Boundary integral equation
- double layer charge
- loop currents
- nonlinear magnetostatic analysis
ASJC Scopus subject areas
- Electrical and Electronic Engineering
- Electronic, Optical and Magnetic Materials
Cite this
Nonlinear magnetostatic analysis by unified BIE utilizing potential gap due to loop currents. / Ishibashi, Kazuhisa; Andjelic, Zoran; Takahashi, Yasuhito; Tawada, Yoshihiro; Yoshioka, Takuya; Wakao, Shinji; Fujiwara, Koji; Ishihara, Yoshiyuki.
In: IEEE Transactions on Magnetics, Vol. 49, No. 5, 6514577, 2013, p. 1573-1576.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Nonlinear magnetostatic analysis by unified BIE utilizing potential gap due to loop currents
AU - Ishibashi, Kazuhisa
AU - Andjelic, Zoran
AU - Takahashi, Yasuhito
AU - Tawada, Yoshihiro
AU - Yoshioka, Takuya
AU - Wakao, Shinji
AU - Fujiwara, Koji
AU - Ishihara, Yoshiyuki
PY - 2013
Y1 - 2013
N2 - Since the line loop current is equivalent to the double layer charge, it gives an integral form of scalar potential. The segmental loop current on the interface between magnetic materials produces a potential gap, which works to give a boundary integral equation (BIE). By virtue of another potential gap due to a fictitious circulating current along the contour of cut-surface in the material, the excitation potential becomes single valued and the BIE becomes applicable to generic problems without any restriction. Regarding the nonlinear magnetic material as composed of segmental materials with different values of permeability, we get the same BIE for the nonlinear analysis as for the linear analysis. In order to check the adequacy and effectiveness of the nonlinear BIE, we solve a typical magnetostatic problem and compare the computed results with those by the conventional magnetic moment method.
AB - Since the line loop current is equivalent to the double layer charge, it gives an integral form of scalar potential. The segmental loop current on the interface between magnetic materials produces a potential gap, which works to give a boundary integral equation (BIE). By virtue of another potential gap due to a fictitious circulating current along the contour of cut-surface in the material, the excitation potential becomes single valued and the BIE becomes applicable to generic problems without any restriction. Regarding the nonlinear magnetic material as composed of segmental materials with different values of permeability, we get the same BIE for the nonlinear analysis as for the linear analysis. In order to check the adequacy and effectiveness of the nonlinear BIE, we solve a typical magnetostatic problem and compare the computed results with those by the conventional magnetic moment method.
KW - Boundary integral equation
KW - double layer charge
KW - loop currents
KW - nonlinear magnetostatic analysis
UR - http://www.scopus.com/inward/record.url?scp=84877863527&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84877863527&partnerID=8YFLogxK
U2 - 10.1109/TMAG.2013.2242434
DO - 10.1109/TMAG.2013.2242434
M3 - Article
AN - SCOPUS:84877863527
VL - 49
SP - 1573
EP - 1576
JO - IEEE Transactions on Magnetics
JF - IEEE Transactions on Magnetics
SN - 0018-9464
IS - 5
M1 - 6514577
ER -