THE MAGNETIC FIELD ABOUT A THREE-DIMENSIONAL BLOCK NEODYMIUM MAGNET

G. Weir, George Chisholm, J. Leveneur
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引用次数: 3

Abstract

Abstract Neodymium magnets were independently discovered in 1984 by General Motors and Sumitomo. Today, they are the strongest type of permanent magnets commercially available. They are the most widely used industrial magnets with many applications, including in hard disk drives, cordless tools and magnetic fasteners. We use a vector potential approach, rather than the more usual magnetic potential approach, to derive the three-dimensional (3D) magnetic field for a neodymium magnet, assuming an idealized block geometry and uniform magnetization. For each field or observation point, the 3D solution involves 24 nondimensional quantities, arising from the eight vertex positions of the magnet and the three components of the magnetic field. The only unknown in the model is the value of magnetization, with all other model quantities defined in terms of field position and magnet location. The longitudinal magnetic field component in the direction of magnetization is bounded everywhere, but discontinuous across the magnet faces parallel to the magnetization direction. The transverse magnetic fields are logarithmically unbounded on approaching a vertex of the magnet.
磁场约为三维块钕磁铁
1984年,美国通用汽车公司和住友汽车公司分别独立发现了钕磁铁。今天,它们是商业上最坚固的永磁体。它们是应用最广泛的工业磁铁,有许多应用,包括硬盘驱动器,无线工具和磁性紧固件。我们使用矢量势方法,而不是更常见的磁势方法,来推导钕磁铁的三维(3D)磁场,假设一个理想的块几何形状和均匀磁化。对于每个场或观测点,三维解涉及24个非量纲量,由磁体的八个顶点位置和磁场的三个分量产生。模型中唯一未知的是磁化强度,所有其他模型量都是根据磁场位置和磁体位置定义的。纵向磁场分量在磁化方向上处处是有界的,但在平行磁化方向的磁体上是不连续的。横向磁场在接近磁体顶点时呈对数无界。
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