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Hard Magnetic Properties of Nanocrystalline Fe-Nd-B Alloys Containing α-Fe and Intergranular Amorphous Phase

机译:含α-Fe和晶间非晶相的纳米晶Fe-Nd-B合金的硬磁性能

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When an amorphous Fe_(90)Nd_7B_3 alloy subjected to annealing for 60 to 180 s at temperatures between 923 and 1023 K consists of a mixed structure of bcc-Fe, Fe_3B, Fe_(14)Nd_2B and remaining amorphous phases, the (BH)_(max) and remanence were found to have maximum values of 113 kJ/ m~3 and 1.17 T, respectively. Their crystallites which precipitated through the process of Am→Am′+bcc-Fe→Am″+bcc-Fe+Fe_3B→Am′′′+bcc-Fe+Fe_3B+Fe_(14)Nd_2B have the particle sizes of 20 to 60 nm and the thickness of the intergranular amorphous layer is 5 to 30 nm. The Fe_(14)Nd_2B phase is surrounded by the bcc-Fe and remaining amorphous phase in the optimally annealed state because it precipitates from the remaining amorphous phase which surrounds the bcc-Fe particles. The further increase in annealing temperature and annealing time causes the increase in particle size of their precipitates as well as the disappearance of the residual amorphous phase, leading to the significant decrease in (BH)_(max). The existence of the residual amorphous phase was also recognized for all other Fe-Nd-B alloys with maximum (BH)_(max) values obtained by annealing the amorphous phase. The intergranular amorphous phase as well as the bcc-Fe phase is presumed to act as an effective magnetic exchange-coupled medium. This information is extremely important for the subsequent development of permanent magnet materials by the utilization of magnetic exchange-coupled state as well as for the interpretation of the appearance of hard magnetism in the use of the rapidly solidified Fe-rich amorphous phase as a precursor.
机译:当在923至1023 K之间的温度下进行60至180 s退火的非晶Fe_(90)Nd_7B_3合金由bcc-Fe,Fe_3B,Fe_(14)Nd_2B和其余非晶相的混合结构组成时,(BH) _(max)和剩磁分别为113 kJ / m〜3和1.17T。通过Am→Am′+ bcc-Fe→Am″ + bcc-Fe + Fe_3B→Am′′′+ bcc-Fe + Fe_3B + Fe_(14)Nd_2B的过程析出的微晶的粒径为20至60层间非晶层的厚度为5〜30nm。 Fe_(14)Nd_2B相在最佳退火状态下被bcc-Fe和剩余的非晶相包围,因为它从围绕bcc-Fe颗粒的剩余非晶相中析出。退火温度和退火时间的进一步增加导致其沉淀物的粒径增加以及残余非晶相的消失,从而导致(BH)_(max)的显着降低。对于所有其他具有通过对非晶态进行退火而获得的(BH)_(max)最大值的Fe-Nd-B合金,也认识到了残余非晶态的存在。晶间无定形相以及bcc-Fe相被假定为有效的磁交换耦合介质。该信息对于随后通过利用磁交换耦合态开发永磁体材料以及对于使用快速凝固的富铁非晶相作为前体来解释硬磁的出现极为重要。

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