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A magnetization table describing the magnetic properties of the material of interest is the primary input for any computer program expected to calculate magnetic fields or other magnetic parameters in a nonlinear case. Magnetization tables, however, consist of discrete points, and the program assumes some interpolation rule to calculate values between them. There exists a variety of interpolation schemes, and some of them can produce very large errors and even unphysical results when the intervals are not narrow enough. Unfortunately, it was found that intervals used in practice are seldom narrow enough. The accurate interpolation of magnetization tables thus becomes a central issue in the numerical solution of nonlinear magnetic problems. We discuss several interpolation schemes used in practice. We propose a new one that is guaranteed to give physical results, and we address the question as to how wide the table invervals can be if a desired accuracy is specified. The discussion is illustrated with many examples.

Infinite elements provide one of the most attractive alternatives for dealing with differential equations in unbounded domains. The region where loads, sources, inhomogeneities and anisotropics exist is modelled by finite elements and the far, uniform region is represented by infinite elements. We propose a new infinite element which can represent any type of decay towards infinity. The element is so simple that explicit expressions can be obtained for the element matrix in many cases, yet large improvements in the accuracy of the solution are obtained as compared with the truncated mesh. Explicit expressions are in fact given for the Laplace equation and 1/rn decay. The element is conforming with linear triangles and bilinear quadrilaterals in two dimensions. The element can be used with any standard finite‐element program without having to modify the shape function library or the numerical quadrature library of the program. The structure or bandwidth of the stiffness matrix of the finite portion of the mesh is not modified when the infinite elements are used. An example problem is solved and the solution found to be better than several other methods in common usage. The proposed method is thus highly recommended.

We present a set of new simple closed‐form analytical formulas for the calculation of the magnetic field produced at any point of space by any solid polyhedral conductor with a uniform current density j. The formulas have been obtained by analytical integration of Ampère's law under the only assumptions that the conductor is bounded by flat surfaces and that j = constant in the conductor. This includes bars, bricks, tetrahedrons, wedges, prisms, trapezoids, pyramids, and polyhedrons in general. The formulas contain no singularities, and can be used for the numerical calculation of the field at any point, including points inside the conductor, or on its surface, edges or corners. The formulas can easily be extended for conductors of infinite length. Extensive numerical tests of the formulas have been performed.