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根据凝固过程中的守恒原理,建立了铝基复合材料凝固过程的数学模型.根据所建立的模型对氧化铝短纤维增强铝铜二元合金复合材料进行数值模拟,模拟结果表明:氧化铝短纤维周围有低熔点物质及溶质富集;随冷却速度增大,复合材料基体偏析加剧;随复合材料中纤维体积分数增大,基体中偏析减小.

参考文献

[1] MORTENSEN A;CORNIE J A .Columnar dendritic solidification in a metal-matrix composite[J].Metallurgical and Materials Transactions,1988,19A:709-721.
[2] A.Sundarrajan;A.Mortensen;T.Z.Kattamis .Kinetic undercooling in solidification of A hypereutectic Al-Si alloy; effect of solidifying within a ceramic preform[J].Acta materialia,1998(1):91-99.
[3] 郭常新,柏善岩.Effects of Cerium on the Mechanical Properties of the ZA22/Al2O3 Composites[J].JOURNAL OF RARE EARTHS,1995(01):27.
[4] MORTENSEN A;JIN I .Solidification processing of metal-matrix composites[J].International Materials Reviews,1992,37(03):101-128.
[5] Park BG.;Hellier AK.;Crosky AG. .Material characterisation and mechanical properties of Al2O3-Al metal matrix composites[J].Journal of Materials Science,2001(10):2417-2426.
[6] 储双杰;吴人洁.挤压铸造莫来石短纤维增强Al-4.5Cu复合材料的凝固组织、偏析及性能的研究[J].铸造,1998(10):4-7.
[7] Al2O3f/Al-4%Cu合金复合材料界面偏析研究[J].热加工工艺,2000(01):18-20.
[8] LI D Z.Modeling of microstructure formation for nickel-based super alloy turbine blade casting[A].,1995:63-74.
[9] 刘政;龚平 .金属基复合材料凝固过程计算机模拟(Ⅰ)[J].南方冶金学院学报,1999,20(02):78-84.
[10] 李强,李殿中,钱百年.Al-7%Si凝固过程组织演变的元胞自动机方法模拟[J].材料工程,2004(07):35-39.
[11] 严卫东,刘汉武,熊玉华,杨爱民,刘林.非定向熔模铸造过程中高温合金叶片晶粒组织的计算机模拟[J].材料工程,2002(04):43-47.
[12] MORTENSEN A;GUNGOR M N;CORNIE J A.Alloy microsegregation in cast metal matrix composites[J].Journal of Metals,1986(03):30-35.
[13] LI Q F;MCCARTNEY D G;WALKER A M .Development of solidification microstructures alloy[J].Journal of Materials Science,1991,26:3565-3574.
[14] MORTENSEN A;CORNIE J A;FLEMINGS M C.Solidification processing of metal-matrix composites[J].Journal of Metals,1988(02):12-19.
[15] KUBO K .Computer simulation of equiaxial dendrite solidification of aluminum alloy[J].Journal of the Japan Institute of Metals,1990,54(07):816-825.
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