利用微观Langevin方程对δ'相(Al3Li)沉淀过程的原子图像进行模拟研究,该方程不但能同时描述原子簇聚和有序化过程,将相分离和粗化在同一物理框架内考虑,而且无须预先设定第二相结构,可观察到动力学演化过程中可能出现的瞬时相.模拟结果表明:对于Al-15Li(原子分数,%)合金,最初在无序基体中出现的L12相浓度与无序相相同,在L12相之间形成重位点阵界面;随后,L12相有序度进一步增加,重位点阵界面逐渐转变为L12结构;最后形成被反相畴界分开的L12结构单相有序相.单相有序相一经形成.便开始分解,分解主要发生在反相畴界处,富Li区向平衡δ'相转化,贫Li区自发无序化,形成δ'相与无序基体共存的平衡结构.在沉淀过程后期.δ'相粗化特征明显,大颗粒长大,小颗粒变小或消失,两相界面由不规则变为平直.
参考文献
[1] | Volmer M, Weber A Z. Phys Chem, 1926; 119:227 |
[2] | Becker R, Doring W. Ann Phys, 1935; 24:719 |
[3] | Turnbull D, Fisher J C. J Chem Phys, 1949; 17:71 |
[4] | Zener C. J Appl Phys, 1949; 20:950 |
[5] | Lifshitz L M, Slyozov V V. J Phys Chem Solids, 1961; 19:35 |
[6] | Wagner C Z F. Elektrochemie, 1961; 65:581 |
[7] | Hassen P. Phase Transformations in Materials. Weinheim: VCH, 1991:281 |
[8] | Cahn J W, Hilliard J E. J Chem Phys, 1958; 28:258 |
[9] | Cahn J W, Hilliard J E. J Chem Phys, 1959; 31:688 |
[10] | Cahn J W. J Chem Phys, 1965; 42: 93 |
[11] | Chen L Q, Khachaturyan A G. Acta Metall Mater, 1991;39:2533 |
[12] | Chen L Q, Khachaturyan A G. Phys Rev, 1991; 44B: 4681 |
[13] | Chen L Q, Khachaturyan A G. Phys Rev, 1992; 46B: 5899 |
[14] | Khachaturyan A G. Theory of Structural Transformations in Solids. New York: Wiley, 1983:139 |
[15] | Noble B, Trowsdale A J. Scr Metall, 1995; 33:33 |
[16] | Lee H Y, Hsu S S, Chen H. Scr Metall, 1991; 25:1549 |
[17] | Schmitz G, Hono K, Haasen P. Acta Metall Mater, 1994;42:201 |
[18] | Mahalingam K, Mahadev V, Liedl G L, Jr Sanders T H.Scr Metall, 1991; 25:2181 |
[19] | Yasuya O, Sadayoshi I, Kiyomichi N. Metall Trans, 1999;30(A): 741 |
[20] | Khachaturyan A G, Lindsey T F, Jr Morris J W. Metall Trans, 1988; 19(A): 249 |
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