2002
DOI: 10.1109/20.996160
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Eddy-current calculations in three-dimensional moving structures

Abstract: A nonconforming nonoverlapping domain decomposition method to approximate the eddy-current problem, formulated in terms of the modified magnetic vector potential, in threedimensional moving structures, is presented. This approximation allows for nonmatching grids at the sliding interface and is based on the mortar element method combined with edge elements in space and finite differences in time. Numerical results illustrate how the method works and the influence of eddy currents on the field distribution.Inde… Show more

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Cited by 19 publications
(14 citation statements)
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“…Based on the mortar edge element method, this approximation has allowed us to work in a very elegant way with domain discretizations that do not match at the interface. The interest of the proposed method is focused on the following issues: (1) the imposition at a discrete level of the transmission condition for the tangential component of the magnetic vector potential field across the interface is done without any constraint between the spatial discretization steps h 1 and h 2 ; (2) the use of second order edge elements on the interface is mandatory to have an optimal approximation of the problem solution; (3) nonmatching grids can be easily intersected by means of a projection procedure based on the introduction of an independent third surface mesh; (4) the system of the discretized problem can be efficiently inverted by a preconditioned conjugate gradient procedure (see [27]). Numerical results confirm the theoretical ones and demonstrate the ability of the proposed method.…”
Section: Discussionmentioning
confidence: 99%
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“…Based on the mortar edge element method, this approximation has allowed us to work in a very elegant way with domain discretizations that do not match at the interface. The interest of the proposed method is focused on the following issues: (1) the imposition at a discrete level of the transmission condition for the tangential component of the magnetic vector potential field across the interface is done without any constraint between the spatial discretization steps h 1 and h 2 ; (2) the use of second order edge elements on the interface is mandatory to have an optimal approximation of the problem solution; (3) nonmatching grids can be easily intersected by means of a projection procedure based on the introduction of an independent third surface mesh; (4) the system of the discretized problem can be efficiently inverted by a preconditioned conjugate gradient procedure (see [27]). Numerical results confirm the theoretical ones and demonstrate the ability of the proposed method.…”
Section: Discussionmentioning
confidence: 99%
“…The method we shall describe and implement here develops what is presented in [3], where the proper space of Lagrange multipliers is defined and optimality of the approximation is proven, and in [9], where a different version of the method is proposed. Moreover, the present analysis is an unavoidable preliminary step to [27] and [11], where the magnetodynamic problem in three-dimensional moving structures is addressed.…”
Section: Domain Decomposition Approachmentioning
confidence: 99%
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“…A different but symmetric approach relies on the introduction of a third discretization on the skeleton, totally independent of those on the mortar and non-mortar sides. A quadrature formula is then defined on the mesh triangles of this third mesh and projected on those of the mortar and non-mortar sides (see [81] for a concrete application of this approach in three dimensions). We refer to [80] for a detailed analysis of the discretization relying on the previous considerations.…”
Section: Construction Of a Basis Of The Constrained Spacesmentioning
confidence: 99%
“…It can provide an efficient formulation for analysis of rotating machinery using a sliding mesh [3] but efficient linear solvers for practical mortar finite element analyses have not been studied sufficiently. This study examines two types of linear systems of equations with and without Lagrange multipliers.…”
Section: Introductionmentioning
confidence: 99%