欢迎登录材料期刊网

材料期刊网

高级检索

采用化学包覆法,以氨水为沉淀剂,在碱性体系中制备了Fe(OH)3包覆T-ZnOw复合粉体,在600℃下通氢气还原获得了Fe/T-ZnOw包覆复合粉体.用XRD,SEM和EDX对粉体进行表征,结果表明:复合粉体存在金属铁相和T-ZnOw相,T-ZnOw四针保持完整,表面包覆完整,铁颗粒为球形,颗粒细小均匀,并T-ZnOw表层外有部分散落铁颗粒,颗粒粒径约为3 μm.用VSM分析测定粉体的磁饱和强度和矫顽力,分别为32.10 emu/g和140.5 Oe.

参考文献

[1] Vladimir B. Bregar .Advantages of Ferromagnetic Nanoparticle Composites in Microwave Absorbers[J].IEEE Transactions on Magnetics,2004(3):1679-1684.
[2] Mizubuehi K;Tanimura H .Fluororesin Composition[P].EP,1584655,2005-10-12.
[3] Zhou Z W;Chu L S;Hu S C et al.Structures of Tetraneedle Like ZnO Whisker During the Crystal Growth[J].Transactions of the Materials Research Society of Japan,2004,29(07):3083-3086.
[4] Z. Zhou;S. Hu;L. Chu .Studies on Tetrapod-Shaped ZnO Whisker Modified Polymer Composites[J].Materials Science Forum,2005(Pt.2):1033-1036.
[5] 楚珑晟,周祚万.氧化锌晶须电磁波吸收性能研究[J].功能材料,2006(01):47-49,53.
[6] Xiaolang Chen;Zuowan Zhou;Kai Wang;Ximei Fan;Shuchun Hu;Yong Wang;Yan Huang .Ferromagnetism In Fe-doped Tetra-needle Like Zno Whiskers[J].Materials Research Bulletin,2009(4):799-802.
[7] O.D. Jayakumar;I.K. Gopalakrishnan;C. Sudakar .Significant enhancement of room temperature ferromagnetism in surfactant coated polycrystalline Mn doped ZnO particles[J].Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics,2007(1/2):258-262.
[8] Hua-Wei Zhang;Zhi-Ren Wei;Zhi-Qiang Li .Room-temperature ferromagnetism in Fe-doped, Fe- and Cu-codoped ZnO diluted magnetic semiconductor[J].Materials Letters,2007(17):3605-3607.
[9] 赵雯,张秋禹,王结良,韩磊,张和鹏.无机粉体化学镀镍的研究进展[J].电镀与涂饰,2004(03):33-36.
[10] 李松梅,陈冬梅,刘建华.T-ZnO晶须化学镀铜复合粉体的制备及其电磁性能的研究[J].物理化学学报,2004(11):1389-1393.
[11] Yu WD;Li XM;Gao XD .Synthesis and structural characteristics of high-quality tetrapodlike ZnO nanocrystals on ZnO and NiO nanocrystal substrates[J].Journal of Crystal Growth,2004(1/2):92-97.
[12] 曲敬信;汪泓宏.表面工程手册[M].北京:化学工业出版社,1998
[13] 庞建明,郭培民,赵沛,曹朝真,张殿伟.低温下氢气还原氧化铁的动力学研究[J].钢铁,2008(07):7-11.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%