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GRAIN BOUNDARY PLANE DISTRIBUTIONS IN RECRYSTALLIZED HIGH PURITY Al AFTER A PARALLEL PROCESSING OF EQUAL CHANNEL ANGULAR PRESSING AND DIRECT ROLLING |
Jixiang CHEN1,Weiguo WANG1,2( ),Yan LIN2,Chen LIN2,Qianting WANG1,2,Pinqiang DAI1,2 |
1 School of Materials Science and Engineering, Fuzhou University, Fuzhou 350108, China 2 School of Materials Science and Engineering, Fujian University of Technology, Fuzhou 350118, China |
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Cite this article:
Jixiang CHEN,Weiguo WANG,Yan LIN,Chen LIN,Qianting WANG,Pinqiang DAI. GRAIN BOUNDARY PLANE DISTRIBUTIONS IN RECRYSTALLIZED HIGH PURITY Al AFTER A PARALLEL PROCESSING OF EQUAL CHANNEL ANGULAR PRESSING AND DIRECT ROLLING. Acta Metall Sin, 2016, 52(4): 473-483.
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Abstract It is quite different from those low to medium stacking fault energy face-centered cubic metals, Al and most its alloys are not applicable to twin-induced grain boundary engineering processing due to their high stacking fault energy. In order to optimize the grain boundary character distribution so as to remarkably better the properties of Al and its alloys, it is necessary at first to study the grain boundary plane distributions. In this work, two parallel high purity (99.99%) Al specimens, which were prepared by multi-directional forging followed by recrystallization annealing resulting in a homogeneous microstructure with averaged grain size around 20 μm, were separately processed by equal channel angular pressing (ECAP) and direct rolling (DR) with true strain ε≈2 followed by a recrystallization annealing at 360 ℃ for 8~90 min. Then, the grain boundary plane distributions were characterized by five-parameter analysis (FPA) based on stereology method and electron backscatter diffraction (EBSD). The results show that the grain boundary planes of the specimens as processed mainly orient on {111}, mostly corresponding to the <111> twist high angle boundaries. It is due to the energy minimum of {111}. The primary difference of grain boundary plane distributions between ECAP and DR specimens lies in the behaviors of grain boundary planes orienting onto {111}. For ECAP specimens, it is slow the grain boundary planes orienting onto {111}. However, for DR specimens, it is quite easy the grain boundary planes orienting onto {111}. Discussions pointed out, compared with ECAP deformation, DR deformation is more efficient for grain boundary plane orienting onto {111} in the subsequent recrystallization annealing and thus is more in favor of the optimization of grain boundary character distribution. It could be attributed to the development of <110>//ND textures during DR deformation which results in the fast grain growth in the subsequent recrystallization annealing.
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Received: 22 July 2015
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Fund: Supported by National Natural Science Foundation of China (Nos.51171095 and 51271058) |
[1] | Watanabe T.Res Mech, 1984; 11: 47 | [2] | Kronberg M L,Wilson F H.Trans AIME, 1949; 185: 501 | [3] | Aust K T, Erb U, Palumbo G.Mater Sci Eng, 1994; A176: 329 | [4] | Chadwick G A, Smith D A.Grain Boundary Structure and Properties. London: Academic Press, 1976: 201 | [5] | Randle V.Scr Mater, 2006; 54: 1011 | [6] | Palumbo G, Erb U.MRS Bull, 1999; 24: 27 | [7] | Xia S, Zhou B X, Chen J W, Wang W G.Acta Metall Sin, 2006; 42: 129 | [7] | (夏爽, 周邦新, 陈觉文, 王卫国. 金属学报, 2006; 42: 129) | [8] | Wang W G, Zhou B X, Feng L.Acta Metall Sin, 2006; 42: 715 | [8] | (王卫国, 周邦新, 冯柳. 金属学报, 2006; 42: 715) | [9] | Wang W G, Zhou B X, Rohrer G S, Guo H, Cai Z X.Mater Sci Eng, 2010; A527: 3695 | [10] | Kumar M, Schwartz A J, King W E.Acta Mater, 2002; 50: 2599 | [11] | Thaveeprungsriporn V, Sinsrok P, Hong-Aram D.Scr Mater, 2001; 44: 67 | [12] | Shimada M, Kokawa H, Wang Z J, Sato Y S, Karibe I.Acta Mater, 2002; 50: 2331 | [13] | Fang X Y, Wang W G, Zhou B X.Acta Metall Sin, 2010; 46: 404 | [13] | (方晓英, 王卫国, 周邦新. 金属学报, 2010; 46: 404) | [14] | Fang X Y, Liu Z Y, Tikhonova M, Belyakov A, Kaibyshev R, Rohrer G S, Wang W G.Acta Metall Sin, 2012; 48: 895 | [14] | (方晓英, 刘志勇, Tikhonova M, Belyakov A, Kaibyshev R, Rohrer G S, 王卫国. 金属学报, 2012; 48: 895) | [15] | Fang X Y, Wang W G, Zhou B X.Rare Met Mater Eng, 2007; 36:1500 | [15] | (方晓英, 王卫国, 周邦新. 稀有金属材料与工程, 2007; 36: 1500) | [16] | McNaughtan D, Worsfold M, Robinson M J.Corros Sci, 2003; 45: 2377 | [17] | Li X L, Chen J H, Liu C H, Feng J N, Wang S H.Acta Metall Sin, 2013; 49: 243 | [17] | (李祥亮, 陈江华, 刘春辉, 冯佳妮, 王时豪. 金属学报, 2013; 49: 243) | [18] | Zhang H F, Zheng Z Q, Zhong S, Luo X F, Zhong J.Trans Nonferrous Met Soc China, 2012; 22: 1025 | [18] | (张海锋, 郑子樵, 钟申, 罗先甫, 钟警. 中国有色金属学报, 2012; 22: 1025) | [19] | Saylor D M, Dasher B E, Rollett A D, Rohrer G S.Acta Mater, 2004; 52: 3649 | [20] | Dong L, Wang W G.Acta Phys Sin, 2013; 15: 42 | [20] | (董垒, 王卫国. 物理学报, 2013; 15: 42) | [21] | Wang W G, Lin C, Li G H, Hua N B, Zhou B X, Fang X Y, Dai P Q, Chen W Z.Sci China, 2014; 44E: 1295 | [21] | (王卫国, 林琛, 李广慧, 花能斌, 周邦新, 方晓英, 戴品强, 陈文哲. 中国科学, 2014; 44E: 1295) | [22] | Segal V M.Mater Sci Eng, 1995; A197: 157 | [23] | Beladi H, Rohrer G S.Metall Mater Trans, 2013; 44A: 115 | [24] | Yu Y N, Liu G Q.Stereologic: Principles and Applications of Quantitative Analysis of Tissue. Beijing: Metallurgical Industry Press, 1989: 123 | [24] | (余永宁, 刘国权. 体视学:组织定量分析的原理和应用. 北京: 冶金工业出版社, 1989: 123) | [25] | Rohrer G S, Saylor D M, Dasher B E, Adams B L, Rollett A D, Wynblatt P.Z Metallkd, 2004; 95: 197 | [26] | Engler O, Huh M.Mater Sci Eng,1999; A271: 371 | [27] | MacKenzie J K.Biometrika, 1958; 45: 229 | [28] | Li J, Dillon S J, Rohrer G S.Acta Mater, 2009; 57: 4304 | [29] | Beladi H, Nuhfer N T, Rohrer G S.Acta Mater, 2014; 70: 281 | [30] | Wen Y N, Zhang J M.Solid State Commun, 2007; 144: 163 |
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