欢迎登录材料期刊网

材料期刊网

高级检索

用单辊快速凝固(RS)薄带在330℃热挤压制备了直径Φ14 mm的AZ91D合金棒材,用OM、SEM、TEM和XRD分析热挤压前后组织的变化,研究了热挤压对其组织与性能的影响.研究发现,热挤压后RS薄带之间焊合良好,挤压态棒材的抗拉强度较普通凝固铸态高55.9%:屈服强度高77.6%;伸长率与铸态相当;维氏硬度和布氏硬度均有较大提高.热处理后,快速凝固挤压棒材的抗拉强度和屈服强度均没有明显变化,伸长率却提高了5.6倍.在RS薄带的挤压过程中过饱和的á-Mg单相固溶体中有少量β-Mg17Al12相脱溶析出,而热处理后有较多细小的β-Mg17Al12相析出,室温拉伸断口呈塑性断裂特征.RS薄带挤压材料的抗拉强度不仅依赖于其本身的微细组织,而且和挤压加工过程密切相关.

参考文献

[1] Polmear I J.Magnesium alloys and application[J].Materials Science and Technology,1994(01):1-16.
[2] Hiroyuki Watanabe;Toshiji Mukai;Masahide Kohzu;Shigenori Tanabe;Kenji Higashi .Low temperature superplasticity in a ZK60 magnesium alloy[J].Materials transactions,1999(8):809-814.
[3] Govind.;Mittal MC.;Lal K.;Mahanti RK.;Sivaramakrishnan CS.;Nair KS. .Development of rapidly solidified (RS) magnesium-aluminium-zinc alloy[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,2001(0):520-523.
[4] 黄正华,郭学锋,张忠明.快速凝固AZ91D镁合金组织的研究[J].材料热处理学报,2005(01):32-35.
[5] 徐锦锋,翟秋亚,袁森.AZ91D镁合金的快速凝固特征[J].中国有色金属学报,2004(06):939-944.
[6] 徐锦锋,翟秋亚.快速凝固AZ91D镁合金的相结构及位错[J].稀有金属材料与工程,2004(08):835-838.
[7] 刘正,范立坤,林立,姜文辉.镁基快速凝固合金的研究与开发[J].汽车工艺与材料,2003(06):20-24.
[8] Guo Xuefeng;Jacob Kinstler;Lilia Glazman.High strength Mg-Zn-Y-Ce-Zr alloy bars prepared RS and extrusion technology[A].北京,2004:20-24.
[9] Hehmann F;So mmer F;Predel B .Extension of solid solubility in magnesium by rapid solidification[J].Materials Science and Engineering A,1990,125:249-265.
[10] Wu Y;Piccone T J;Shiohara Y et al.Dendritic growth of undercooled nickel-tin Part Ⅰ[J].Metallurgical and Materials Transactions A:Physical Metallurgy and Materials Science,1987,18:915-924.
[11] Piccone T J;Wu Y;Shiohara Y et al.Dendritic growth of undercooled nickel-tin Part Ⅱ[J].Metallurgical and Materials Transactions A:Physical Metallurgy and Materials Science,1987,18:925-932.
[12] M. MABUCHI;K. HIGASHI .STRENGTHENING MECHANISMS OF Mg-Si ALLOYS[J].Acta materialia,1996(11):4611-4618.
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%