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根据γ-TiAl层状晶体(PST晶体)的微观结构,构造了可使用有限元计算的夹心基元。由有限元计算表明,当裂尖平行于片层时,裂尖前端所有滑移系上的分切应力都很小,即滑移较弱,而沿片层界面(它总是解理面之一)的正应力有最大值,这表明,裂尖将沿片层扩展,而且塑性小。当裂纹垂直于片层时,裂尖前端很多滑移系上的分切应力都很大,最大正应力并不在片层界面上,而总在跨片层的解理面上,这表明,裂尖在片层内解理,并且塑性很大。

参考文献

[1] Kim Y W;Dimiduk D M .Progress in the Understanding of Gamma Titanium Aluminides[J].Journal of The Minerals,Metals & Materials Society,1991,8:40.
[2] Masahurn Yamaguchi;Haruyuri Inui.TiAl Compounds for Structural Application[A].USA:The Minerals Metals and Materials Society,1993:127.
[3] 陆永浩,张永刚,乔利杰,王燕斌,陈昌麒,褚武扬.全层状TiAl基合金断裂机制原位观察[J].稀有金属材料与工程,2001(01):15-18.
[4] Umakoshia Y;Nakano T .The Role of Ordered Domains and Slip Mode of α2 Phase in the Plastic Behavior of TiAl Crystal Containing Oriented Lamellar[J].冶金材料学报,1993,41(04):1155.
[5] France S;Coujou A;Coumet A .An In Situ Study of Twin Propagation in TiAl[J].Philosophical Magazine,1993,67(01):127.
[6] Yamaguchi M .High Temperature Intermatallics-with Particular Emphasis on TiAl[J].Materials Science and Technology,1992,8:299.
[7] 王继杰,蒋敏,郝士明.γ-TiAl基双相合金片层组织不连续粗化的驱动力与动力学[J].稀有金属材料与工程,1998(03):161-164.
[8] 曹国鑫,林建国,孙志鹏,张永刚,陈昌麒.晶粒尺度和片层厚度对全片层γ-TiAl合金性能的影响[J].稀有金属材料与工程,2000(03):172-176.
[9] S. YOKOSHIMA;M. YAMAGUCHI .FRACTURE BEHAVIOR AND TOUGHNESS OF PST CRYSTALS OF TiAl[J].Acta materialia,1996(3):873-883.
[10] Lipsitt H A;Shechtman D;Schafrik R E.The Deforma tion and Fracture of TiAl at Elevated Temperatures[J].Metallurgical and Materials Transactions A:Physical Metallurgy and Materials Science,1975(06):1991.
[11] Sun Y Q;Hazzledine P M;Christian J M .Intersections of Deformation Twins in TiAl[J].Philosophical Magazine A:Physics of Condensed Matter:Structure,Defects and Mechanical Properties,1993,68(03):495.
[12] Yoo MH.;Fu CL.;Zou J. .MECHANISTIC MODELING OF DEFORMATION AND FRACTURE BEHAVIOR IN TIAL AND TI3AL[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,1995(0):14-23.
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