欢迎登录材料期刊网

材料期刊网

高级检索

采用修正的嵌入原子模型(modified embedded atom method,(MEAM)),给出了Cu,Ag,Au,Ni,Pd,Pt,Rh,Ir等元素的所有嵌入原子参数,用所给参数计算了上述元素的单空位形成能、双空位结合能、结构能量差及由它们构成的二元合金的稀溶解热.计算的稀溶解热与实验结果及已有的理论计算结果进行了比较,现在的计算值与已有的实验结果和Miedema理论计算结果符合得比较好.

参考文献

[1] Daw M S et al.[J].Physical Review B,1984,29:6443.
[2] Bangwei Z et al.[J].Physical Review B,1993,48:3022.
[3] Yifang O et al.[J].Transactions Nfsoc,1998,8:60.
[4] Wangyu H et al.[J].Journal of Physics D:Applied Physics,2000,33:711.
[5] Wangyu H et al.[J].Journal of Alloys and Compounds,1999,287:159.
[6] F. Fang;X. L. Shu;H. Q. Deng .Modified analytic EAM potentials for the binary immiscible alloy systems[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,2003(1/2):357-367.
[7] Yifang O et al.[J].ZPhysikB,1996,101:161.
[8] Bangwei Z et al.[J].Journal of Materials Science and Technology,1999,15:331.
[9] Yifang O et al.[J].Journal of Materials Science and Technology,2003,19:243.
[10] Clementi E;Roetti C.Atomic Data and Nuclear Data Tables[M].New York:Academic Press,1974:428.
[11] Kittle C.Introduction to Ssolid State Physics[M].New York:John Wiley & Sons,1986:55.
[12] Miedema A R .[J].Zeitschrift fur Metallkunde,1979,70:345.
[13] Herman H;Ullmaier H.Landolt-Bornstern[M].Heideberg:Springer-Verlag,1983
[14] Johnson R A .[J].Physical Review B,1989,39:12554.
[15] Baskes M I .[J].Physical Review B,1992,46:2727.
[16] Goreckl T .[J].Zeitschrift fur Metallkunde,1974,65:426.
[17] Drittler B et al.[J].Solid State Communications,1991,79:31.
[18] Baskes M I et al.[J].Physical Review B,1979,20:3197.
[19] Keegan M A et al.[J].Physical Review B,1995,51:17431.
[20] Lam N Q et al.[J].Journal of Physics F:Metal Physics,1985,15:799.
[21] Bakker H.Enthalpies in Alloys[M].Switzerland:Trans Tech Publications Ltd,1998
[22] Hultgren R.Selected Values of the Thermodynamic Properties of Binary Alloys[M].New York:American Society for Metals,1973
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%