材料科学
矫顽力
剩磁
凝聚态物理
各向异性
铁氧体(磁铁)
幂律
磁晶各向异性
磁滞
法学
磁各向异性
磁化
复合材料
磁场
物理
光学
统计
量子力学
数学
政治学
作者
Fernando José Gomes Landgraf,M. Emura,Marcos Flávio de Campos
标识
DOI:10.1016/j.jmmm.2008.04.011
摘要
The behavior of the Steinmetz coefficient has been described for several different materials: steels with 3.2% Si and 6.5% Si, MnZn ferrite and Ni–Fe alloys. It is shown that, for steels, the Steinmetz law achieves R2>0.999 only between 0.3 and 1.2 T, which is the interval where domain wall movement dominates. The anisotropy of Steinmetz coefficient for non-oriented (NO) steel is also discussed. It is shown that for a NO 3.2% Si steel with a strong Goss component in texture, the power law coefficient and remanence decreases monotonically with the direction of measurement going from rolling direction (RD) to transverse direction (TD), although coercive field increased. The remanence behavior can be related to the minimization of demagnetizing field at the surface grains. The data appear to indicate that the Steinmetz coefficient increases as magnetocrystalline anisotropy constant decreases.
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