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Microstructure and Properties of Die-Upset Nd-Fe-B/Dy$_{2}$ O$_{3}$ Composite Magnets

机译:模锻Nd-Fe-B / Dy $ _ {2} $ O $ _ {{3} $)复合磁体的组织和性能

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Fabrication of rare-earth-based permanent magnets with both high electrical resistivity and excellent magnetic properties for the traction motor applications is highly challenging. In this paper, Nd-Fe-B/Dy $_{2}$O $_{3}$ composite magnets have been fabricated by hot-pressing and die-upset. The influence of Dy $_{2}$O $_{3}$ filler on the microstructures, electrical resistivity and magnetic properties of the Nd-Fe-B magnets have been investigated by scanning electron microscope, four-probe resistivity meter and hysteresis graph. The results showed that the electrical resistivities of the Nd-Fe-B/Dy$_{2}$ O$_{3}$ composite magnets increased with the increase of Dy $_{2}$O $_{3}$ amount and reached 1270 $mu Omega$ cm when the Dy$_{2}$O$_{3}$ amount increased to 20 wt.%. Whereas the electrical resistivity of the nondoped Nd-Fe-B magnets is 230 $mu Omega$ cm. The cross-section SEM images of the composite magnets showed that the Dy$_{2}$ O$_{3}$ phase formed laminated structure and some agglomerate phenomenon. The agglomerate areas became larger with the in- rease of Dy $_{2}$O $_{3}$ amount. The residual magnetic flux density $({rm B}_{rm r})$ and maximum energy product of the Nd-Fe-B/Dy $_{2}$O $_{3}$ composite magnets decreased due to the nonmagnetic Dy$_{2}$ O$_{3}$ filler. It is interesting to find that coercivity of the Nd-Fe-B/Dy$_{2}$O $_{3}$ composite magnets increased from 7.8 kOe to 9.64 kOe when the Dy$_{2}$ O$_{3}$ amount increased from 10 wt.% to 20 wt.%. The reason may be that some of the dysprosium diffused into the Nd-Fe-B matrix and formed (Nd,Dy)$_{2}$Fe$_{14}$B compounds. In the mean time, some of neodymium-rich phase diffused to Dy $_{2}$O $_{3}$ phase, replaced dysprosium and formed Nd$_{2}$O$_{3}$. This probably happened during the die-upset process at 850 $^{circ}$C.
机译:对于牵引电动机应用而言,具有高电阻率和优异磁性能的稀土基永磁体的制造是极具挑战性的。在本文中,Nd-Fe-B / Dy <分子式type =“ inline”> $ _ {2} $ O <分子式type =“ inline”> $ _ {3} $ 复合磁体是通过热压和模锻加工而成的。 Dy $ _ {2} $ O $ _ {3} $ 填充剂对Nd-Fe-B磁体的微观结构,电阻率和磁性能的影响。结果表明,Nd-Fe-B / Dy <公式公式类型=“ inline”> $ _ {2} $ O <公式公式的电阻率=“ inline”> $ _ {3} $ 复合磁体随着Dy $ _ {2} $ O $ _ {3} $ 金额达到1270当Dy $ _时, $ mu Omega $ cm {2} $ O $ _ {3} $ 的数量增加到20 wt。% 。而未掺杂的Nd-Fe-B磁体的电阻率为230 <配方公式= inline“> $ mu Omega $ cm。复合磁体的横截面SEM图像显示,Dy $ _ {2} $ O $ _ {3} $ 相形成了层状结构和一些团聚现象。随着Dy $ _ {2} $ O $ _ {3} $ 金额。剩余磁通量密度<公式公式类型=“ inline”> $({rm B} _ {rm r})$ 和Nd-的最大能量积Fe-B / Dy $ _ {2} $ O $ _ {3} $ 复合磁体由于非磁性Dy $ _ {2} $ 而减少 O $ _ {3} $ 填充符。有趣的是,发现Nd-Fe-B / Dy <分子式的矫顽力 $ _ {2} $ O <分子式当Dy $ _ {3} $ 复合磁体从7.8 kOe增加到9.64 kOe。 =“ TeX”> $ _ {2} $ O $ _ {3} $ 量从10重量%增加到20重量%。原因可能是某些扩散到Nd-Fe-B基质中并形成(Nd,Dy)<分子式 $ _ {2} $ Fe $ _ {14} $ B化合物。同时,一些富钕相扩散到Dy $ _ {2} $ O $ _ {3} $ 相,置换了and并形成了Nd $ _ {2} $ O $ _ {3} $ 。这可能是在850 $ ^ {circ} $ C的换模过程中发生的。

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