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Self-diffusion in Υ-TiAl: an experimental study and atomistic calculations

机译:Υ-TiAl中的自扩散:实验研究和原子计算

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摘要

This paper presents the results of combinedexperiemental and theoretical studies of Ti self-diffusion in theintermetallic compound Υ-TiAl. Ti self-diffusion coefficientswere measured over a temperature range of 1184-1691 K usingthe radiotracer 44Ti and the serial sectioning method. Thediffusion coefficients show a non-Arrhenius behaviour withsignificant upward deviations at high temperatures(above~1470K). The pre-exponential factor and the activationenergy of self-diffusion determined in rthe low temperaturerange (<1470 K) are (DTi)0≈1.5×10-6m2/s and QTi≈250kJ/mol,respectively. By combining the obtained Ti selfdiffusioncoefficients with interdiffusion coefficients measured previouslyby Sprengel et al. (W.Sprengel, N. Opkawa, H. Nakajima,intermetallics 4 (1996), 185) and using the Darken-Manningequation, Al self-diffusion coefficients in TiAl were evaluated.Within the scatter of the data points, Al self-diffusion followsthe Arrhenius law with (DAl)0≈2.1×10-2m2/sand QAl≈360kJ/mol. The energies of point defect formation andmigration in TiAl were calculated by molecular statics withembedded-atom potentials. Several diffusion mechanisms inTiAl were considered, including migration of Ti and Al alongtheir own sublattices by single vacancy jumps, 3-jump vacancycycles and the anti-structural bridge mechanism. The activationenergies of Ti and Al self-diffusion by different mechanismswere evaluted as functions of the alloy composition. Thecaculations predict that, in the compositions studiedexperimentally, Ti diffusion at low temperatures is dominated bythe vacancy mechanism ,while at higher temperatures the anti-structural bridg mechanism can essentially contribute to theoverall diffusivity. Al diffusion occurs by the vacancymechanism with some contribution of 3-jump cycles and anti-structural bridges. The se predictions are in good agreementwith the experimental results of this work
机译:本文介绍了金属间化合物Υ-TiAl中Ti自扩散的实验和理论研究相结合的结果。使用放射性示踪剂44Ti和连续切片法在1184-1691 K的温度范围内测量Ti的自扩散系数。在高温(〜1470K以上)下,扩散系数显示出非阿累尼乌斯行为,且具有明显的向上偏差。在低温范围(<1470 K)中确定的指数前因子和自扩散活化能分别为(DTi)0≈1.5×10-6m2 / s和QTi≈250kJ/ mol。通过将获得的Ti自扩散系数与Sprengel等人先前测得的互扩散系数相结合。 (W.Sprengel,N.Opkawa,H.Nakajima,intermetallics 4(1996),185)并使用Darken-Manningequation评估了TiAl中Al的自扩散系数。遵循阿累尼乌斯定律,(DAl)0≈2.1×10-2m2 / s和QAl≈360kJ/ mol。 TiAl中点缺陷形成和迁移的能量是通过具有嵌入原子电势的分子静力学来计算的。考虑了TiAl中的几种扩散机制,包括Ti和Al通过单空位跃迁,3跳空位循环和抗结构桥机制沿其自身的亚晶格迁移。钛和铝通过不同机制自扩散的活化能被评估为合金成分的函数。计算表明,在实验研究的成分中,空位机理主导了低温下的Ti扩散,而在较高温度下,抗结构桥联机理可基本促进总体扩散。铝的扩散是由空位机理引起的,具有3级跳跃循环和抗结构桥的作用。这些预测与这项工作的实验结果非常吻合

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