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The Third Group of Spacial Distribution of Magnetic Leakage Field Yielded by A Rectangular Slot on The Workpiece Surface

机译:由工件表面上的矩形槽产生的磁漏场的第三组空间分布

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The objective of this study was to explain quantitatively a surprising phenomenon?a?athe magnetic polarity in a slot on the workpiece surface after discontinuation of longitudinal magnetization is opposite to it, when the specimen is being magnetized, that is,the magnetic residual field shows negative values. On the basis of uniform distribution of magnetic charges along all edges of a cuboid magnetic medium in the stable condition of magnetization and the demagnetization law of ferromagnetic materials( after removal of magnetizing field the difficult degree of the returning of a magnetic dipole back to its original orientation before magnetization depends on the magnitude of the mechanical reacting force and mechanical moment affected by this magnetic dipole in stable condition of magnetization ),they are known that after discontinuation of longitudinal magnetization rear magnetic charges excited during the magnetization may be remained along the bottom edges of the throughout rectangular slot on a cuboid steel component,and that there will appear unlike magnetic charges opposite to those,which had existed at the magnetization along the rest edges and over the lateral surfaces of the slot. Thereby this strange phenomenon was clarified. The spacial distribution gragh of the magnetic leakage field calculated and plotted along the symmetrical axis of the slot basically conformed to the third group of curves obtained from Dr. F. F.rster?ˉs experiment made in 1985.
机译:本研究的目的是定量解释令人惊讶的现象?当样品被磁化时,在停止纵向磁化后的工件表面上的槽中的磁极性在工件表面上的磁极性与其相对。即,当样品被磁化时,即磁残留场显示负值。基于磁性磁介质的所有边缘均匀分布磁化的磁化强度的稳定条件和铁磁材料的退磁定律(除去磁化磁场后,磁性偶极的难度返回其原始磁化前的取向取决于受该磁性偶极物影响的机械反应力和机械时刻在磁化的稳定条件下的幅度),因此已知在停止在磁化期间激励的纵向磁化后磁性电荷之后可以沿着底部边缘留下在长方体钢部件上的整个矩形槽中,并且将出现与沿着其余边缘的磁化在磁化处的磁性电荷相反的磁性电荷不同。从而澄清了这种奇怪的现象。沿着槽的对称轴计算和绘制的磁漏电场的间隔分布格栅基本上符合从F.F.Rster博士获得的第三组曲线αˉS实验1985年。

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