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Revisiting the demagnetization curves of Dy-diffused Nd-Fe-B sintered magnets

机译:重新探测Dy扩散ND-Fe-B烧结磁体的退磁曲线

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The grain boundary diffusion process (GBDP) is now widely used to increase coercivity in Nd-Fe-B sintered magnets with a more efficient use of heavy rare earth elements (Dy, Tb). This process leads to a typical core-shell structure for the grains consisting of (Nd,Dy)_2Fe_(14)B shells at the outer grain regions and Nd_2Fe_(14)B cores. The thickness of the (Nd,Dy)_2Fe_(14)B shells decreases from the diffusion surface to the magnet core. This inhomoge-neous distribution in Dy content gives rise to a coercivity gradient within the magnet and leads therefore to a reduced squareness of the demagnetization curve. The purpose of this work is to provide a quantitative understanding of the influence of composition profiles after GBDP on the shape of the demagnetization curve of Nd-Fe-B sintered magnets diffused with the Dy_(63)Co_(37) (at. %) intermetallic compound. SEM/X-EDS analyses along the Fisher diffusion model allow the estimation of the Dy concentration in grains and at different depths. Then, after ascribing to the grains some critical values for the switching field that are related to the local Dy content, a macroscopic finite element model is implemented to provide a better understanding of the grain reversal sequence in the graded magnets tested in closed-circuit. Grain reversal patterns show that demagnetization starts from the less coercive grains in the magnet core, remains constricted in this zone thanks to a shielding effect from the external surface, and then propagates towards outer layers via magnetostatic interactions. When the coercivity gradient is large, the coercivity of the whole magnet measured in closed-circuit could be 100-200 kA/m lower than the value expected without considering magnetostatic interactions, suggesting that the shielding effect from the diffusion affected layers could be limited and counterbalanced by magnetostatic interactions.
机译:晶界扩散过程(GBDP)现在广泛用于增加ND-Fe-B烧结磁体中的矫顽力,具有更有效地使用重稀土元素(Dy,Tb)。该方法导致典型的芯壳结构,用于包括在外晶粒区域的(Nd,Dy)_2fe_(14)B壳体中的颗粒和Nd_2Fe_(14)B芯。 (ND,Dy)_2Fe_(14)B壳的厚度从扩散表面到磁芯的厚度降低。这种在Dy含量的Inhomoge - 奈多分布产生磁体内的矫顽力梯度,因此引入降低的去磁曲线的大方形。本作作品的目的是提供对GBDP在与DY_(63)CO_(37)扩散的ND-Fe-B烧结磁体的退磁曲线形状的形状的形状中的数量理解。(63)CO_(37)(AT.%)金属间化合物。沿着Fisher扩散模型分析SEM / X-EDS分析允许估计晶粒和不同深度的Dy浓度。然后,在归因于谷物归因于与局部DY内容相关的切换场的一些临界值之后,实现了宏观有限元模型,以便在闭合电路中测试的渐变磁体中的晶粒反转序列更好地理解。晶粒反转图案表明,由于来自外表面的屏蔽效果,从磁芯芯中的胁迫颗粒仍然在该区域中仍然限制,然后通过磁静物相互作用朝向外层传播。当矫顽力梯度大时,在闭合电路中测量的整个磁体的矫顽力可以是100-200kA / m的预期而不考虑静磁相互作用,这表明来自扩散受影响的层的屏蔽效果可能是有限的通过磁化相互作用进行平衡。

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