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液态金属Ga急冷凝固中微观结构转变的模拟研究
引用本文:张海涛,刘让苏,陈晓莹,杜生海,侯兆阳,张爱龙.液态金属Ga急冷凝固中微观结构转变的模拟研究[J].原子与分子物理学报,2005,22(3):449-455.
作者姓名:张海涛  刘让苏  陈晓莹  杜生海  侯兆阳  张爱龙
作者单位:湖南大学应用物理系,长沙,410082
基金项目:国家自然科学基金资助项目(50271026)
摘    要:采用分子动力学方法对液态金属Ga的快速凝固过程进行计算机模拟跟踪研究,运用HA键型指数法和原子团类型指数法分析了金属原子Ga的成键类型和形成的基本原子团结构.发现:与通常的液态金属(如Al)相反,随着温度的降低,二十面体及与二十面体相关的1551, 1541键型数目明显下降;与立方体(fcc,bcc),六角密集结构相关的1421,1422键型数目明显增加;而与菱面体相关的1321,1311键型的数目却显著增加,逐渐占据优势.最后形成一种新型的以菱面体结构为主、夹杂着立方体(fcc,bcc)、六角密集(hcp)等团簇结构所组成的非晶态结构.这正是非晶态金属Ga的g(r)曲线分裂的第二峰的顺序为前低后高,而与非晶态金属Al的g(r)曲线(其分裂的第二峰的顺序为前高后低)明显不同的微观结构上的物理根源.

关 键 词:液态金属Ga  微结构转变  团簇结构  分子动力学  计算机模拟
文章编号:1000-0364(2005)03-0449-07
收稿时间:02 15 2005 12:00AM
修稿时间:2005-02-15

Simulation study of microstructure transition of liquid metals Ga during rapid cooling solidifications
ZHANG Hai-tao,LIU Rang-su,CHEN Xiao-rong,DU Sheng-hai,HOU Zhao-yang,ZHANG Ai-long.Simulation study of microstructure transition of liquid metals Ga during rapid cooling solidifications[J].Journal of Atomic and Molecular Physics,2005,22(3):449-455.
Authors:ZHANG Hai-tao  LIU Rang-su  CHEN Xiao-rong  DU Sheng-hai  HOU Zhao-yang  ZHANG Ai-long
Abstract:A computer simulation tracking study for the rapid solidification proc esses of liquid metal Ga system has been performed by using molecular dynamics method. Adopting the Honeycutt-Andersen (HA) bond-type index method and the cluster-type index met hod, the bond-types and the basic cluster configurations formed by metal Ga atoms are analyzed. It has been found that, contrary to conventional metals (such as Al), with decreasing temperature, the number of ico sahedron and the relative numbers of 1551,1541 bond types related to the icosahedron decreased obviously; the total number of 1421, 1422 bond types, related to the cubic (fcc, bcc) and hcp structures increased ob viously; and the total number of 1311, 1301 bond types, related to the rhombohedral stru cture, increased remarkably, and gradually played a dominant role. Finally, an amorphous structure was forme d mainly with rhombohedral structures and mixed up with clusters of cubic (f.c.c, b.c.c) a nd h.c.p structures. This is just the physical origin in microstructure for the obvious difference between the g (r) curves of amorphous metal Ga having a splitting second peak with a lower front sub-peak and a higher behi nd one, with those of amorphous metal Al having a splitting second peak with a higher front sub-peak and a lower behind one.
Keywords:Liquid metal Ga  Microstructure transition  Cluster structure  Mol ecular dynamics  Computer simulation
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