利用微观相场动力学模型模拟研究873 K时Ni75CrxAl25-x合金中Cr原子的替代规律.在合金沉淀过程中,Cr原子部分替代Al原子格点形成Ll2结构的γ相(Ni75CrxAl25-x).Cr原子在L12相内的占位几率极限值较小,当Cr含量超过3%时,Li2相内Cr原子的浓度接近饱和值.在Li2相的有序畴界处,Cr原子完全取代Al原子位置,形成稳定的Ni3Cr相(DO22结构).该合金最终沉淀产物为Ni75CrxAl25-x混合相.
参考文献
[1] | Liu ZH;Liu H;Zhang XX;Zhang M;Dai XF;Hu HN;Chen JL;Wu GH .Martensitic transformation and magnetic properties of Heusler alloy Ni-Fe-Ga ribbon[J].Physics Letters, A,2004(3):214-220. |
[2] | 卢艳丽,陈铮,李永胜,王永欣.含共格畸变的立方合金粗化机制的原子层面计算机模拟研究[J].稀有金属材料与工程,2006(11):1686-1690. |
[3] | 赵宇宏,张跃,陈铮.Ni75Al4V21合金沉淀早期微观相场法模拟[J].北京航空航天大学学报,2007(08):978-981. |
[4] | Jiri Cermak;Ales Gazda;Vera Rothova .Interdiffusion in ternary Ni_3Al/Ni_3Al-X diffusion couples with X =Cr, Fe, Nb and Ti[J].Intermetallics,2003(9):939-946. |
[5] | Mekhrabov A O;Akdeniz M V;Arer M M .[J].Acta Materialia,1997,45(03):1077. |
[6] | Ochiai S;Oya Y;Suzuki T .[J].Acta Metallurgy,1984,32(02):289. |
[7] | Marry A;Bessiere M;Bley F .[J].Acta Metallurgica Et Materialia,1990,38(02):345. |
[8] | Pareige C;Soisson F;Martin G .[J].Acta Metallurgica Et Materialia,1999,47(06):1889. |
[9] | Chen L Q;Khachamryan A G .[J].Scripta Metallurgica et Materialia,1991,25(01):61. |
[10] | Chen L Q;Khachaturyan A G .[J].Acta Metallurgica Et Materialia,1991,39(11):2533. |
[11] | Chen Longqing .[J].Scripta Metallurgica et Materialia,1993,20(05):683. |
[12] | Raable D.Computational Materials Science[M].北京:化学工业出版社,2002:223. |
[13] | Khachatuyran A G.Theory of Structural Transformations in Solids[M].New York:wiley,1983:23. |
[14] | Poduri R;Chen L Q .[J].Acta Materialia,1998,46(03):1719. |
[15] | Zhang J X;Chen L Q .[J].Acta Materialia,2005,53(05):2845. |
[16] | Seol D J;Hu S Y;Li Y L et al.[J].Acta Materialia,2003,51(10):5173. |
[17] | CHU Zhong,CHEN Zheng,WANG Yong-Xin,LU Yan-Li,ZHANG Jian-Jun.Microscopic Phase-Field Simulation of Atom Substitution Behaviour in Ni-Cr-Al Alloy[J].中国物理快报(英文版),2005(08):1841-1844. |
[18] | Blavette D;CadaE l;Deconihout B .[J].Materials Characterization,2000,44(11):133. |
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:
-
10%
-
20%
-
30%
-
40%
-
50%