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1998
DOI: 10.1109/20.717718
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A novel formulation for 3D eddy current problems with moving bodies using a Lagrangian description and BEM-FEM coupling

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Cited by 68 publications
(44 citation statements)
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“…the term γ v × (∇ × A) becomes dominant and causes instabilities in the numerical solution process [24]. In (2.16), h denotes the discretization parameter in direction of the velocity v. However, if due to mechanical movements/deformations the overall magnetic field is changed (e.g., movement of the armature in a magnetic valve), we have to consider the formulation of the magnetic problem on the deformed geometry [24].…”
Section: The Magnetic System and The Coupling Termsmentioning
confidence: 99%
See 1 more Smart Citation
“…the term γ v × (∇ × A) becomes dominant and causes instabilities in the numerical solution process [24]. In (2.16), h denotes the discretization parameter in direction of the velocity v. However, if due to mechanical movements/deformations the overall magnetic field is changed (e.g., movement of the armature in a magnetic valve), we have to consider the formulation of the magnetic problem on the deformed geometry [24].…”
Section: The Magnetic System and The Coupling Termsmentioning
confidence: 99%
“…In (2.16), h denotes the discretization parameter in direction of the velocity v. However, if due to mechanical movements/deformations the overall magnetic field is changed (e.g., movement of the armature in a magnetic valve), we have to consider the formulation of the magnetic problem on the deformed geometry [24]. Observing some point P in a fixed reference frame Γ (x, y, z) (see Fig.…”
Section: The Magnetic System and The Coupling Termsmentioning
confidence: 99%
“…In the case of moving bodies the equations (2) and (3) change accordingly to the movement law (see [19] for a short presentation) and we consider the formulation in term of Lagrangian variables.…”
Section: Problem Equations In the Case Of Moving Geometriesmentioning
confidence: 99%
“…In electromagnetic scattering, a major challenge is overcoming problems with pollution (dispersion) error in wave propagation. In terms of low frequency electromagnetics, such as electromagnetic radiation in low frequency devices such as MRI scanners, the eddy current approximation of the full Maxwell system can be adopted [216,113,37,141,206], which requires special treatment through gauging conditions on the equations [153]. In the eddy current approximation, a major challenge lies in the accurate resolution of the small skin depths in conductors due to higher frequency excitations.…”
Section: Approaches For Electromagneticsmentioning
confidence: 99%
“…The simulation of MRI scanners also builds on the expanding literature devoted to magneto-mechanics and coupled problems including FEM-BEM coupling [125,141], magneto-mechanical damping machines [40], magneto-mechanical effects on material parameters [133], enhanced basis functions for magneto-mechanical coupling [107] and strongly coupled systems [204]. More specifically, attempts to analyse the magneto-mechanical coupling in MRI systems have been considered; with the modelling of axisymmetric superconducting solenoids in self magnetic fields [101] and efficient low order FE solvers for magneto-mechanical coupling in [202], based on the FEM-BEM program CAPA [126], with extensions also to include acoustic effects [203].…”
Section: Applications To Mri Scannersmentioning
confidence: 99%