2009
DOI: 10.1109/tmag.2008.2005119
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Magnetic Field Analysis of an Arbitrary Shaped Coil Using Shape Functions

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Cited by 20 publications
(17 citation statements)
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“…Equations (A7)-(A12) are determined from boundary conditions. As shown in Figure 1, when an arbitrarily shaped coil, which is positioned at z = z 0 and carrying current I, the x-, y-and z-components of magnetic flux densityb i (ξ, η, z) at z < z 0 are described as follows [14] b ix = μ 0 Iξ 2η e …”
Section: Appendix Amentioning
confidence: 99%
“…Equations (A7)-(A12) are determined from boundary conditions. As shown in Figure 1, when an arbitrarily shaped coil, which is positioned at z = z 0 and carrying current I, the x-, y-and z-components of magnetic flux densityb i (ξ, η, z) at z < z 0 are described as follows [14] b ix = μ 0 Iξ 2η e …”
Section: Appendix Amentioning
confidence: 99%
“…Other authors have proposed different methods to calculate the current and power density distributions, e.g., using an impedance matrix [6], [11] or with finite element computation of the electromagnetic problem [7], [9], [19]- [21]. In this paper, this last method is used for the calculation of the power density curve induced in a C-45 steel disk with a diameter of 0.1 m, using a circular inductor with the same size in a centered position, heating with a total power of 1 W. In this case, the power distribution is symmetrical with respect to the center of the disk and constant in the azimuthal direction [ Fig.…”
Section: Theoretical Model Of Temperature Distributionmentioning
confidence: 99%
“…where the power density in the region, Dp,i, is obtained from the power density distribution of the inductor, calculated in [12]- [ 14] with finite element analysis. An example of the power density distribution of an inductor with a diameter of .…”
Section: It Theoretical Analysis Of Heat Distributionmentioning
confidence: 99%