论文

冷却速率对GWZ1032K合金中14H-LPSO结构形成的影响

  • 张松 ,
  • 袁广银 ,
  • 丁文江 ,
  • 卢晨
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  • 1.上海交通大学材料科学与工程学院 轻合金精密成型国家工程研究中心, 上海 200240
    2.上海交通大学材料科学与工程学院 金属复合材料国家重点实验室, 上海 200240
张松, 男, 1983年生, 博士生

收稿日期: 2010-04-14

  修回日期: 2010-07-14

  网络出版日期: 2010-10-11

基金资助

上海市基础研究重点项目08JC141412200, 新世纪优秀人才支持计划项目NCET-07-0554和江苏省先进金属材料高技术研究重点实验室开放课题项目AMM200903资助

EFFECT OF COOLING RATE ON THE FORMATION OF 14H–LPSO STRUCTURE IN GWZ1032K ALLOY

  • ZHANG Song ,
  • YUAN An-Yin ,
  • DING Wen-Jiang ,
  • LV Chen
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  • 1. Light Alloy Net Forming National Engineering Research Center, School of Materials Science and Engineering, Shanghai
    Jiao Tong University, Shanghai 200240
    2, The State Key Laboratory of Metal Matrix Composite, School of Materials Science and Engineering, Shanghai
    Jiao Tong University, Shanghai 200240

Received date: 2010-04-14

  Revised date: 2010-07-14

  Online published: 2010-10-11

Supported by

Supported by Science and Technology Commission of Shanghai Municipality (No.08JC141412200), Program for New Century Excellent Talents in University (No.NCET–07–0554), and Open Research Fund Program by Jiangsu Key Laboratory of Advanced Metallic Materials (No.AMM200903)

摘要

采用金属型铸造和慢速凝固, 在不同冷却速率下制备了Mg-10Gd-3Y-1.8Zn-0.5Zr(质量分数, %) (GWZ1032K)合金. 采用SEM, TEM和XRD研究了冷却速率不同的GWZ1032K 合金的组织和相构成. 在GWZ1032K合金中, α-Mg基体中的层片状14H-LPSO结构随着冷却速率的下降而增加, 在冷却速率为0.005℃/s的试样中充满了整个晶粒;随着合金冷却速率降低, GWZ1032K合金中晶界第二相分别由5℃/s时的(Mg, Zn)3RE相转变为0.5 和0.1℃/s时的(Mg, Zn)3RE相和14H-LPSO结构的χ相共存;在0.01和0.005℃/s时只有14H-LPSO结构的$\chi$相. 结果显示在接近于平衡凝固的缓慢冷速条件下, 更容易形成具有稳定结构的层片状14H-LPSO结构和χ相.在冷却速率为0.5和0.1℃/s时, (Mg, Zn)3RE共晶相和χ相共存, (Mg, Zn)3RE共晶相和χ相的位向关系为 [110]χ phase//[223](Mg, Zn)3RE和∠g(001)χ phase g(110) (Mg, Zn)3RE=8.4°.

本文引用格式

张松 , 袁广银 , 丁文江 , 卢晨 . 冷却速率对GWZ1032K合金中14H-LPSO结构形成的影响[J]. 金属学报, 2010 , 46(10) : 1192 -1199 . DOI: 10.3724/SP.J.1037.2010.00177

Abstract

Mg–10Gd–3Y–1.8Zn–0.5Zr (mass fraction, %) (GWZ1032K) alloys were fabricated by permanent mold casting and slow solidification with different cooling rates. The microstructures of the GWZ1032K alloys with different cooling rates were investigated by SEM, TEM and XRD. Two kinds of LPSO structure were observed, include lamellar 14H–LPSO structure in the grain interior and χ phase at the grain boundaries. Lamellar 14H–LPSO structure in α–Mg matrix propagated in the matrix with the decease of solidification rate, and filled the whole grain in the alloy solidified at 0.005 ℃/s. The second phase in the alloys also changed with deceasing the solidification rates, there are (Mg, Zn)3RE compounds only when solidification rate is 5 ℃/s, (Mg, Zn)3RE compounds and 14H–LPSO structured  phase when solidification rates are 0.5 and 0.1 ℃/s, and 14H–LPSO structured χ phase only when solidification rates are 0.01 and 0.005 ℃/s. It was detected that (Mg, Zn)3RE compounds and χ phase existed simultaneously at the grain boundaries in the alloys at solidification rates of 0.5 ℃/s and 0.1℃/s, and the orientation relationship between them was determined to be [110] χphase//[223](Mg,Zn)3RE and ∠g(001)χ phase g(110) (Mg, Zn)3RE=8.4°.

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