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首页> 外文期刊>Journal of Materials Science >TRANSFORMATION TOUGHENING IN THE GAMMA-TIAL-BETA-TI-V SYSTEM .2. A MOLECULAR DYNAMICS STUDY
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TRANSFORMATION TOUGHENING IN THE GAMMA-TIAL-BETA-TI-V SYSTEM .2. A MOLECULAR DYNAMICS STUDY

机译:GAMMA-TIAL-BETA-TI-V系统中的转化强化2。分子动力学研究

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Molecular dynamics simulations of the evolution of materials in a region surrounding a crack tip were carried out for the case of a crack in a gamma-TiAl phase impinging at a rig ht ang le onto the interface between a gamma-TiAl phase and a metastable Ti-15V (at %) phase. The corresponding linear anisotropic solutions for the singular stress and displacement fields were used to both generate the crack in the original crystal and to prescribe the boundary conditions applied to the computational crystal during the molecular dynamics simulation runs. The atomic interactions were accounted for using appropriated embedded atom method (EAM) type interatomic potentials. The crack-tip behaviour for the two-phase gamma-beta material was ultimately compared with the one in the corresponding single-phase material, i.e. to the one in pure gamma and the one in pure beta crystals. The simulation results showed that under the same applied level of external stress, the crack tip became blunt and the crack stopped propagating in the gamma-TiAl-beta-Ti-15V bicrystal and in the single beta-phase crystal while the crack extended by brittle cleavage in the single-phase gamma crystal. The blunting process was found to be controlled by the martensitic transformation that took place in the beta-phase ahead of the crack tip. Depending on the local stress conditions the crystal structure of martensite was found to be either hexagonal close packed (h.c.p.), body centred orthorhombic (b.c.o.) and/or face centred orthorhombic (f.c.o.). Finally the implications of crack tip martensitic transformation on the toughness of the materials are analysed in quantitative terms using the concept of Eshelby's conservation integral, i.e. the energy release rate. [References: 36]
机译:对于γ-TiAl相中的裂纹以一定角度撞击到γ-TiAl相和亚稳Ti之间的界面的情况,对裂纹尖端周围区域中材料的演化进行了分子动力学模拟。 -15V(at%)相。奇异应力场和位移场的相应线性各向异性解既用于在原始晶体中生成裂纹,又用于规定在分子动力学模拟过程中应用于计算晶体的边界条件。使用适当的嵌入原子方法(EAM)类型的原子间电势来解释原子间的相互作用。最终将两相γ-β材料的裂纹尖端行为与相应的单相材料中的裂纹尖端行为进行了比较,即与纯γ晶体中的一种和纯β晶体中的一种比较。仿真结果表明,在相同的外加应力水平下,裂纹尖端变钝,裂纹在γ-TiAl-β-Ti-15V双晶和单β相晶体中停止扩展,而裂纹扩展为脆性在单相伽马晶体中裂解。发现钝化过程受裂纹尖端前β相中发生的马氏体转变控制。根据局部应力条件,发现马氏体的晶体结构为六方密堆积(h.c.p.),体心斜方晶(b.c.o.)和/或面心斜方晶(f.c.o.)。最后,利用埃舍尔比守恒积分的概念(即能量释放率),定量分析了裂纹尖端马氏体相变对材料韧性的影响。 [参考:36]

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