2012
DOI: 10.1049/iet-smt.2011.0216
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Electromagnetic fields generated by arbitrarily shaped current loops

Abstract: New expressions for the magnetic and electric fields generated by arbitrarily shaped current loops are presented. The expressions pertain to all points in space outside the current conductor. Vector magnetic potential and certain first derivatives are calculated without recourse to field solvers; subsequent calculations yield magnetic flux density and electric field intensity. Understanding current loops finds application in fields including recording, medicine and weapons.

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Cited by 2 publications
(1 citation statement)
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“…The eddy-current magnetic flux density can be obtained according to Equations (11), i.e., the Boit–Savart–Laplace law [17,18]:dBeddy=μ0Iunit4πnormalditaliclfalse˜unit×italicDfalse˜italic0italicunitDunit2 where Iunit is the unit-element current; dtruel˜unit—unit length of unit-element current; Dunit—distance between unit-element current and the checkpoint; trueD˜0unit—unit vector from unit-element current to the checkpoint; dBeddy—unit magnetic field that unit-element current generated on the watch point.…”
Section: Anisotropic Surface Conductivity Of the Rotormentioning
confidence: 99%
“…The eddy-current magnetic flux density can be obtained according to Equations (11), i.e., the Boit–Savart–Laplace law [17,18]:dBeddy=μ0Iunit4πnormalditaliclfalse˜unit×italicDfalse˜italic0italicunitDunit2 where Iunit is the unit-element current; dtruel˜unit—unit length of unit-element current; Dunit—distance between unit-element current and the checkpoint; trueD˜0unit—unit vector from unit-element current to the checkpoint; dBeddy—unit magnetic field that unit-element current generated on the watch point.…”
Section: Anisotropic Surface Conductivity Of the Rotormentioning
confidence: 99%