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Boundary conditionsThe physical model would lead us to a problem in an infinite domain with Sommerfeld's radiation condition, cf. [10]. However, in many practical cases we may assume that the field lines of the magnetic induction do not enter or leave a bounded domain representing the device (e.g. the machine). The latter condition, called flux-surface condition, requires that the normal component vanishes on the boundary which is assumed to be sufficiently smooth, i.e.Suppose for the moment that the normal direction is in the z direction of the Cartesian coordinate system. Then we have and is an immediate consequence of Therefore, we will demand that the tangential components of vanish on , i.e. If (12) holds on a smooth surface, then we get
if and denote two perpendicular tangential unit vectors. Thus, in view of (5), we should formulate a Neumann condition for the normal component rather than a Dirichlet condition. Before we discuss the interface conditions, we perform the standard procedure for getting a variational formulation from (8), i.e. we multiply with a test function v and obtain The second integral will be zero if , i.e. . The latter will be satisfied if is taken from an appropriate test space related to , see Subsection 3.1. |
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