The crystallographic features of pearlite were investigated by experiments and edge-to-edge matching principle. Two new orientation relationships between ferrite and cementite were determinated by selected area electron diffraction and then explained by our modified edge-to-edge matching method. The consistence of the experimental results with theoretical prediction confirms the practicability of the modified edge-to-edge matching model.
参考文献
[1] | N. Nakada;N. Koga;T. Tsuchiyama .Crystallographic orientation rotation and internal stress in pearlite colony[J].Scripta materialia,2009(2):133-136. |
[2] | S.TAGASHIRA;K. SAKAI .Deformation Microstructure and Tensile Strength of Cold Rolled Pearlitic Steel Sheets[J].ISIJ International,2000(11):1149-1155. |
[3] | Y.S. Yang;J.G.Bae;C.G. Park .Nanostructure and mechanical properties of heavily cold-drawn steel wires[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,2009(1/2):148-155. |
[4] | J.LANGUILLAUME;G.KAPELSKI;B.BAUDELET .CEMENTITE DISSOLUTION IN HEAVILY COLD DRAWN PEARLITIC STEEL WIRES[J].Acta materialia,1997(3):1201-1212. |
[5] | M.-X.Zhang;P.M.Kelly .Crystallography of spheroidite and tempered martensite[J].Acta materialia,1998(11):4081-4091. |
[6] | M.-X. Zhang;P.M. Kelly .Edge-to-edge matching and its applications. Part II. Application to Mg-Al, Mg-Y and Mg-Mn alloys[J].Acta materialia,2005(4):1085-1096. |
[7] | M.-X. Zhang;P.M. Kelly .Edge-to-edge matching and its applications. Part I. Application to the simple HCP/BCC system[J].Acta materialia,2005(4):1073-1084. |
[8] | M.-X. ZHANG;S.-Q. CHEN;H.-P. REN .Crystallography of the Simple HCP/FCC System[J].Metallurgical and materials transactions. A, physical metallurgy and materials science,2008(5):1077-1086. |
[9] | M.-X. ZHANG;P.M. KELLY .Edge-to-edge matching model for predicting orientation relationships and habit planes -- the improvements[J].Scripta materialia,2005(10):963-968. |
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%