本文采用多相流模型对不同冷却条件下Al-Si/SiC系统二维凝固过程进行了数值模拟,对顶面冷却、底面冷却、侧面冷却和四面冷却条件下,无颗粒、小颗粒和大颗粒的情况进行了研究.溶质分布表明:对于分凝系数小于1的合金,先凝固的地方出现负偏析,后凝固的地方出现正偏析.顶面冷却和底面冷却时会出现A型偏析,侧面冷却和四面冷却时出现V型偏析.共晶分布验证了Scheil方程,共晶的产生会受到宏观偏析的影响,而且大颗粒的堆积会抑止共晶的产生.
参考文献
[1] | Gao J W, Wang C Y. Solidification processing of functionally graded materials by sedimentation [A]. Proceedings of ASME Heat Transfer Division [C]. 1999. 1-13. |
[2] | Feller R J, Beekermann C. Solidification of metal-matrix composites with convection [J]. Metall and Mater Trans B,1997,28B(6): 1165- 1183. |
[3] | 杜卓林,陈义良,黄庆,等.重力作用下Al-Si/SiC颗粒系统二维凝固过程数值模拟[J].中国科学技术大学学报,2002,32(3) :293-301. |
[4] | Ding J, Gidaspow D. A bubbling fluidization model using kinetic theory of granular flow [J]. American Institute of Chemical Engineers Journal, 1990, 36(4): 523-538. |
[5] | Gidaspow D. Hydrodynamics of fluidization and heat transfer:supercomputer modeling [J]. Appl Mech Rev, 1986, 39(1): 1-23. |
[6] | Shih Y T,Gidaspow D,Wasan D T. Hydrodynamics of sedimentation of multisized particles [J]. Powder Technol, 1987,50(3):201-215. |
[7] | Wang C Y, Beckermann C. A multiphase solute diffusion model for dendritic alloy solidification [J]. Metall Trans A,1993,24A(12): 2787-2802. |
[8] | Kurts W, Fisher D J. Fundamentals of Solidification [M].Switzerland, Aedermannsdorf: Trans Tech Publications,1999. |
[9] | Rohatgi P K, Pasciak K, Narendranath C S, et al. Evolution of microstructure and local thermal conditions during directional solidification of A356-SiC particle composites [J]. J Mater Sci, 1994,29(20):5357-5368. |
[10] | Voller V R. Fast implicit finite-difference method for the analysis of phase change problems [J]. Numerical Heat Transfer, Part B,1990, 17(2):155-169. |
[11] | Schneider M C, Beckermann C. A numerical study of the combined effects of microsegregation, mushy zone permeability and contraction driven flow on macrosegregation and eutectic formation in binary alloy solidification [J]. Iht J Heat Mass Transfer, 1995, 38(18):3455-3473. |
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%