首页> 外文会议>International symposium on magnetic anisotropy and coercivity in rare-earth transition metal alloys >The Role of Integranular Regions in Sintered Nd-Fe-B Magnets with (B.H)_max>420 kJ/m~3 (52.5 MGOe)
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The Role of Integranular Regions in Sintered Nd-Fe-B Magnets with (B.H)_max>420 kJ/m~3 (52.5 MGOe)

机译:(B.H)_MAX> 420 kJ / m〜3(52.5 MgOE)中,在烧结ND-Fe-B磁体中的角度在烧结ND-Fe-B磁体中的作用

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Anisotropic Nd-Fe-B magnets with a high remanence and energy density were produced by powder metallurgy. In order to obtain an energy density of (B.H)_max >420 kJ/m~3 a minimum coercive field of _JH_c>750 kA/m is necessary. Experimental investigations have shwon that hte improving alignment of the grains decreases the coercive field of the sintered magnets. It was found that abnormal grain growth preferentially occurs in magnets with a higher degree of mislaignment. 3-dimensional micromagnetic simulations show that the intergranular region between the graisn, which is determined by the composition of the magnets and the annealing treatment, plays a significant role determining the magnetic properties. The coercivity is determiend by the long range dipolar interaction and short range exchagne coupling between neighbouring grains. The numerical finite element simulations show that assuming a disturbed intergranular region of about 5 to 10 nm with a reduced magnetocrystalline anisotropy the calculated coercive field is reduced to comparable experimetnal values of _JH_c<1000 kA/m. The micromagnetic simulations further show that in the case of a reduced anisotropy between the hard magnetic grains the nucleation of reversed domains starts at the grain boundaries, and the coercive field increases with decreasing alignment of the hard magnetic grains in the range of 8 deg to 16 deg misalignment.
机译:具有高剩磁和能量密度的各向异性ND-Fe-B磁体由粉末冶金生产。为了获得(B.H)_MAX> 420kJ / m〜3的能量密度,需要_jh_c> 750ka / m的最小矫顽区域。实验研究具有SHWON,改善晶粒的对准降低了烧结磁体的矫顽磁场。结果发现,在具有更高程度的计量程度的磁体中优先发生异常的晶粒生长。三维微磁模拟表明,通过磁体的组成和退火处理确定的GRAISN之间的晶间区域起到确定磁性的重要作用。通过在相邻谷物之间的长距离偶极相互作用和短程跃装耦合来确定矫顽力。数值有限元模拟表明,假设具有降低的磁镀晶各向异性的约5至10nm的干扰晶间区域,计算的矫顽磁场减少到_jh_c <1000ka / m的可比实验值。微磁性模拟进一步表明,在硬磁性晶粒之间的各向异性的情况下,反向域的成核在晶界开始,并且矫顽场随着8°至16的范围内的硬磁颗粒的对准而增加Deg Misalignment。

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