The calculation and graphic imaging of magnetic charge density provides fresh insights into old problems in micromagnetics. (1) The full saturation magnetization Msof polycrystalline iron can be used in a transformer when magnetic charge at the grain boundaries suppresses the adverse effects of anisotropy. A single domain wall separates two regions of opposite magnetization |M| = Msin toroidal geometry. This is a three-dimensional expression of the ripple effect, long known in polycrystalline thin films of Permalloy. (2) Helical patterns of M result from interaction of regions of opposite magnetic charge developed by the introduction of some ∇ · M when the exchange energy primarily invokes ∇ × M to accommodate to the boundary conditions set by geometry and surface charge density n · M. The helical structures resolve 40-year-old mysteries in the appearance of periodic stripe domains associated with the propagation of edge solitons in a hexagonal [1 1 1] oriented iron whisker.
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A. S. Arrott (2016) studied this question.
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