基于微观相场动力学模型,对应变诱发镍基合金粗化过程共格沉淀相的形貌不稳定性及其发展规律进行了研究.结果表明,应变能作用下,粗化过程中沉淀颗粒界面曲率发生变化,通过沿[10]方向尺寸减小与[11]方向尺寸增大,转变为方形.低应变能作用下,沉淀颗粒形貌由圆形转变为周边圆滑,边长向外凸的方形颗粒;中等应变能作用下,沉淀颗粒形貌由圆形变为边长向内凹的方形;高应变能作用下,圆形沉淀颗粒先转变为方形,再从方形颗粒中心“分裂”为2个长条状颗粒,进一步转变为双透镜形状.
参考文献
[1] | Motejadded H B;Soltanieh M;Rastegari S .[J].Journal of Materials Science and Technology,2012,28(03):221. |
[2] | Muralidharan G;Chen H .[J].Science and Technology of Advanced Materials,2000,1(01):51. |
[3] | 侯介山,郭建亭,周兰章,叶恒强.K44镍基高温合金长期时效过程中γ'相粗化对拉伸性能的影响[J].金属学报,2006(05):481-486. |
[4] | Qiu Y Y .[J].Acta Metallurgica,1996,44:4969. |
[5] | Minoru D;Miyazaki T;Teruyuki W .[J].Materials Science and Engineering,1984,67(02):247. |
[6] | Chen L Q .[J].Annual Review of Materials Research,2002,32:113. |
[7] | 李永胜,陈铮,卢艳丽,王永欣,褚忠.Ni-Al-V合金有序畴界面结构的微观相场模拟[J].稀有金属材料与工程,2006(02):200-204. |
[8] | Moelanes N;Blanpain B;Patrick W .[J].CALPHAD-Computer Coupling of Phase Diagrams and Thermochemistry,2008,32(02):268. |
[9] | Dorr, M.R.;Fattebert, J.-L.;Wickett, M.E.;Belak, J.F.;Turchi, P.E.A. .A numerical algorithm for the solution of a phase-field model of polycrystalline materials[J].Journal of Computational Physics,2010(3):626-641. |
[10] | Hu S Y;Chen L Q .[J].Acta Materialia,2001,49:1879. |
[11] | Poduri R;Chen L Q .[J].Acta Materialia,1997,45(01):245. |
[12] | Prikhodko S V;Carnes J D;Isaak D G et al.[J].Scripta Materialia,1998,38(01):67. |
[13] | Khachaturyan A G;Semenovskays S V;Morris J W .[J].Acta Materialia,1988,36(06):1563. |
[14] | 冯端.相交,金属物理学,第2卷[M].北京:科学出版社,2000:122. |
[15] | Qiu YY. .The splitting behavior of gamma ' particles in Ni-based alloys[J].Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics,1998(1/2):145-153. |
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