利用轻气炮装置在不同加载速率下对Ni47Ti44Nb9形状记忆合金进行了动态冲击加载试验.采用差示扫描量热仪(DSC)、X射线衍射仪(XRD)和透射电子显微镜(TEM)等先进手段对样品的形变行为进行了分析表征.探讨冲击过程合金样品的物相转变机制和微观组织演化规律.结果表明:冲击后样品内部存在大量微观缺陷,NiTi基体相与β-Nb粒子相均发生了明显的形变,但未发生应力引发马氏体相变过程,这可能是由于Ni47Ti44Nb9合金马氏体相变温度较低以及β-Nb粒子对相变过程的阻碍作用引起的.
参考文献
[1] | Ottavia Corbi.Shape memory alloys and their application in structural oscillations attenuation[J].Simulation modelling practice and theory: International journal of the Federation of European Simulation Societies,20035/6(5/6):387-402. |
[2] | Es-Souni M;Es-Souni M;Fischer-Brandies H.Assessing the biocompatibility of NiTi shape memory alloys used for medical applications[J].Analytical and bioanalytical chemistry,20053(3):557-567. |
[3] | L. WANG;L.J. RONG;D.S. YAN.DSC study of the reverse martensitic transformation behavior in a shape memory alloy pipe-joint[J].Intermetallics,20053/4(3/4):403-407. |
[4] | 何向明;戎利建;闫德胜;姜志民;李依依.形变对Ti44Ni47Nb9宽滞后形状记忆合金应力诱发马氏体相变行为的影响[J].金属学报,2004(7):721-725. |
[5] | 颜莹;金伟;曹名洲.Ni47Ti44Nb9形状记忆合金冷轧管材的组织、织构和相变[J].金属学报,2008(2):139-144. |
[6] | J.C.F. Millett;N.K. Bourne.The shock-induced mechanical response of the shape memory alloy, NiTi[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,20041/2(1/2):138-142. |
[7] | Meziere YJE;Millett JCF;Bourne NK.Equation of state and mechanical response of NiTi during one-dimensional shock loading[J].Journal of Applied Physics,20063(3):33513-1-33513-8-0. |
[8] | A.M.Thakur;N.N.Thadhani.Shock-Induced Martensitic Transformations in Near-Equiatomic NiTi Alloys[J].Metallurgical and Materials Transactions, A. Physical Metallurgy and Materials Science,19977(7):1445-1454. |
[9] | T. Kurita;H. Matsumoto;K. Sakamoto.Transformation behavior of shock-compressed Ni_(48)Ti_(52)[J].Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics,20051/2(1/2):92-95. |
[10] | 颜莹;金伟;邱绍宇.热处理对Ti44Ni47Nb9合金的组织和MS点的影响[J].材料研究学报,2004(2):199-204. |
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