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A computational model coupling an electromagnetic model with a macroscopic heat and fluid flow model in semisolid Al alloy slung prepa-ration by A-EMS was developed.The effects of A-EMS processing parameters such as stirring current,stirring frequency and stirring gap width on macroscopic transport phenomena during solidification were analyzed.Both the computational and experimental results showed that more intensively uniform stirring fields and uniformly fine microstructures were obtained by optimizing processing variables.

参考文献

[1] Xu J;Zhang Z.F;Bai Y.L;Shi L.K .The Method and Apparatus for Preparing the Semisolid Rheo-slurry or Billets[P].Chinese Patent,Appl.2008101161819,2008.
[2] Zhang Z.F;Xu J;Bai Y.L;Shi L.K .Development of rheo-diecasting of Al-Si alloys based on a modified DSCP process[J].Solid State Phenomena,2008,141-143:185.
[3] BAI Yue-long,XU Jun,ZHANG Zhi-feng,SHI Li-kai.Annulus electromagnetic stirring for preparing semisolid A357 aluminum alloy slurry[J].中国有色金属学报(英文版),2009(05):1104-1109.
[4] Guanglei ZHU,Jun XU,Zhifeng ZHANG,Yuelong BAI,Likai SHI.Annular electromagnetic stirring-a new method for the production of semi-solid A357 aluminum alloy slurry[J].金属学报(英文版),2009(06):408-414.
[5] 7.hang Z.F;Xu J;Shi L.K .Study on multiple electrn-magnetic continuous casting of aluminum alloy[J].Materials Science and Technology,2006,22(04):437.
[6] 陈兴润,张志峰,徐骏,石力开.环缝式电磁搅拌法制备半固态浆料过程电磁场的数值模拟[J].北京科技大学学报,2009(10):1305-1310.
[7] 陈兴润,张志峰,徐骏,石力开.电磁搅拌法制备半固态浆料过程电磁场、流场和温度场的数值模拟[J].中国有色金属学报,2010(05):937-945.
[8] Zhang Z.F;KIM J.M;Hong C.P .Numerical simulation of grain struct}ue evolution in solidification of an Al-5.Owt% Cu alloy under electromagnetic stirring and its experimental verification[J].ISIJ International,2005,45(02):183.
[9] 刘政,毛卫民,赵振铎.新工艺制备半固态A356铝合金浆料[J].金属学报,2009(04):507-512.
[10] Z. Fan;Y. Wang;M. Xia .Enhanced heterogeneous nucleation in AZ91D alloy by intensive melt shearing[J].Acta materialia,2009(16):4891-4901.
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