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国家自然科学基金(50801049)

作品数:8 被引量:21H指数:3
相关作者:李军刘颖马毅龙高静杜慧龙更多>>
相关机构:四川大学更多>>
发文基金:国家自然科学基金四川省科技攻关计划更多>>
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8 条 记 录,以下是 1-8
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化学气相沉积法制备Nd-Fe-B/α-Fe纳米复合磁体
2010年
采用化学气相沉积法制备单质铁包覆Nd-Fe-B复合磁粉, 经放电等离子烧结得到Nd-Fe-B/α-Fe纳米复合磁体。SEM、XRD、XPS研究表明:采用化学气相沉积法可以实现纳米单质铁对Nd-Fe-B磁粉表面的均匀包覆,有效地改善软硬磁性相的分布,提高磁体的综合磁性能。化学气相沉积温度为120 ℃、沉积时间为30 min时,得到的包覆层致密均匀,单质铁颗粒尺寸50-100 nm。在优化工艺条件下制备出接近全致密的纳米复合磁体,其磁性能可达:Br=0.81 T, Hcj=1286 kA/m , (BH)m =108.6
高静刘颖李军马毅龙杜慧龙高升吉
关键词:化学气相沉积放电等离子烧结
放电等离子烧结法制备的Nd-Fe-B/α-Fe纳米复合磁体
2009年
采用放电等离子烧结和化学气相沉积技术制备烧结型Nd-Fe-B/α-Fe纳米复合磁体,并对磁体的密度、微结构、磁性能进行了分析与表征。研究表明,采用Fe(CO)5热分解化学气相沉积法能实现纯净的纳米单质铁对磁粉表面的均匀包覆,并得到Nd-Fe-B/α-Fe纳米复合磁粉,包覆的纳米铁颗粒尺寸仅为50nm左右。将复合磁粉经放电等离子烧结,可实现快速致密化,当烧结温度达700℃,Nd-Fe-B/α-Fe纳米复合磁体已接近全致密,其晶粒大小约为100nm。该磁体的综合磁性能达到:Br=0.79T,Hcj=1201kA/m,Hcb=507kA/m,(BH)max=103 kJ/m3。
高静刘颖李军马毅龙杜慧龙高升吉涂铭旌
关键词:放电等离子烧结化学气相沉积微结构磁性能
放电等离子烧结温度对热压/热变形NdFeB纳米晶永磁体磁性能的影响被引量:4
2010年
采用放电等离子烧结技术制备了热压/热变形NdFeB磁体。研究了不同烧结温度对热压磁体、热变形磁体微观结构及磁性能的影响。结果表明,随烧结温度的升高,磁体密度上升,680℃时已达理论密度的99.7%;另一方面,晶粒则随温度的增加发生长大。剩磁和最大磁能积受密度和晶粒大小的交互作用,在650℃时达最大:(BH)m=129kJ/m3,Br=0.87T,Hci=914kA/m。热变形后,磁体主相晶粒的c轴逐渐转向与压力平行的方向,形成磁晶各向异性,使磁体的剩磁和最大磁能积大幅增加。热压烧结温度对热变形磁体的磁性能有着极大影响,其剩磁和最大磁能积随热压温度的升高先升高后降低,620℃热压后,热变形磁体磁性能达最大:(BH)m=339kJ/m3,Br=1.49T,Hci=576kA/m。
李超英刘颖李军马毅龙谢发尹周晓庆
关键词:放电等离子烧结技术热变形NDFEB磁体
放电等离子烧结制备纳米晶双相耦合(NdDy)_(11.5)(FeCoNb)_(82.4)B_(6.1)致密磁体
2009年
使用放电等离子烧结(SPS)制备致密的纳米晶交换耦合Nd2Fe14B/α-Fe永磁合金。研究烧结温度、时间、压力对合金磁性能和显微组织的影响。结果表明,随温度、压力的升高,密度增大,磁能积增加;但温度过高或时间过长,使得晶粒长大,导致矫顽力降低。在烧结压力为500MPa,烧结温度为700℃保温3min后,得到密度为7.6g/cm3,晶粒细小的致密块体,其磁性能为:Br=0.81T,Hci=856kA·m-1,(BH)m=106kJ·m-3,其晶粒大小约20nm。
马毅龙刘颖李军杜慧龙高静高升吉
关键词:纳米晶放电等离子烧结显微组织
Microstructure and magnetic properties of bulk magnets Nd_(14-x)Fe_(76+x)Co_3Zr_1B_6(x=0,0.5,1) prepared by spark plasma sintering被引量:3
2009年
Melt-spun ribbons with nominal composition of Nd14–xFe76+xCo3Zr1B6(x=0,0.5,1) were consolidated into isotropic bulk magnets by spark plasma sintering method.It was found that the Nd content and sintering temperature had significant influence on the density and magnetic properties of the sintered magnets.Homogeneous microstructure and fine grain(50–100 nm) were obtained when sintering below 700 ℃,and the initial magnetization curve showed that the coercivity was controlled by the pinning mechanism.However,ab...
马毅龙刘颖李军杜慧龙高静
关键词:MICROSTRUCTURE
放电等离子烧结制备的Nd_2Fe_(14)B/α-Fe复合永磁材料被引量:1
2009年
采用粉末混合技术和放电等离子烧结制备出各向同性Nd2Fe14B/α-Fe复合磁体。Fe的加入使磁体的剩磁增强,矫顽力降低。当(NdDy)14Fe79.5Ga0.5B6中Fe粉添加量达到5wt%时,磁体综合性能最佳:Br=0.84T,Hcj=1474kA/m,(BH)max=105.3kJ/m3。当Fe含量大于5wt%时,由于Fe的团聚严重,α-Fe与基体相Nd2Fe14B作用效果降低,从而导致磁体磁性能降低,退磁曲线呈明显的两相特征。为进一步提高磁体性能,对含5wt%Fe粉的热压磁体进行热变形,形变量为70%,与不含Fe粉的热变形磁体相比,剩磁有所提高,而矫顽力下降很大,磁体(BH)max从231kJ/m3提高到266kJ/m3。
杜慧龙刘颖马毅龙李军高静徐建川涂铭旌
关键词:放电等离子烧结热变形磁性能
Enhanced magnetic properties in Nd-Fe-B magnets prepared by spark plasma sintering via die-upsetting process被引量:8
2011年
The magnetic properties and microstructure of Nd-Fe-B magnets prepared by spark plasma sintering with different die-upsetting processes were investigated. The results showed that the optimum magnetic properties of die-upset Nd-Fe-B magnets were obtained at 680 ℃ when the die-upset level was 60%, and the degree of magnetic alignment was 0.84. The microstructures showed that the coarse grains oc-curred predominantly within certain areas, and abnormal grain growth was not observed within the major areas of well-aligned grains. There existed many small spherical grains, which stacked together and were not aligned during die upsetting when the deformation temperature was 650 ℃. These small spherical grains grew up, and were aligned when the deformation temperature increased from 650 to 680 ℃, which could improve the crystallographic alignment of die-upset Nd-Fe-B magnets.
胡志华储林华李军刘颖
Enhanced mechanical properties in die-upset Nd-Fe-B magnets via die-upsetting process被引量:7
2012年
The mechanical properties of die-upset Nd-Fe-B magnets produced at different die-upset processes were investigated. The results showed that the optimum comprehensive mechanical properties of die-upset Nd-Fe-B magnets were obtained at the deformation temperature of 680 ℃. The anisotropy of Vickers hardness was more obvious at the die-upset level of 55%, and the Vickers hardness measured parallel to the c-axis was significantly lower than that perpendicular to the c-axis. The fracture toughness measured parallel to the c-axis first increased, and then decreased with increase in die-upset level. The maximum fracture toughness of Nd-Fe-B magnets was obtained at the die-upset level of 60%. The microstmcture showed that the width of defect layers and the average size of large grains increased, and the layered structure of die-upset Nd-Fe-B magnets was obviously different with increase in the die-upset level.
胡志华瞿海锦赵佳奇罗成李军刘颖
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