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This model consists of a very thin single turn coil (2(2 mm) with an inner radius of 50 mm. It has been used to compare the solution of femme with the analytic result for a circular current.
This model consists of the above described thin single turn coil and a model of the field coil, which is used in the experimental setup.
This model includes the simplified model of the field coil (only one big turn) and a cylinder with a radius of 2 mm and a height of 8 mm.
This model includes the simplified model of the field coil (only one big turn) and spheres with radii of 2.5, 3.65, and 5 length units.
This model includes the simplified model of a field coil (only one big thin turn) at a larger distance and spheres with radii of 2.5, 3.65, and 5 length units.
This model includes the above described cylinder and the detailed model of the field coil (4(24 turns) used in the experimental setup.
This model includes the detailed coil model and three spheres (radius of 2.5, 3.6 mm, and 5 cm) for the spherical Cu and Al samples. Furthermore, it has been used to compare the solution of femme with the analytic result for the eddy currents in a solid Fe sphere [7].
This model includes the simplified model of a field coil (only one small thin turn) at a short distance.
This model is the same assphere.FEM, but the radius of the boundary, where asymptotic boundary conditions are applied, is doubled.
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