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首页> 外文期刊>Acta Materialia >QUANTITATIVE ANALYSIS OF OBSERVATIONS ON DIFFUSION INDUCED GRAIN BOUNDARY MIGRATION FOR RANDOM BOUNDARIES IN THE Cu(Zn) SYSTEM USING A DRIVING FORCE MODEL
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QUANTITATIVE ANALYSIS OF OBSERVATIONS ON DIFFUSION INDUCED GRAIN BOUNDARY MIGRATION FOR RANDOM BOUNDARIES IN THE Cu(Zn) SYSTEM USING A DRIVING FORCE MODEL

机译:利用驱动力模型对Cu(Zn)系统中随机边界的扩散诱发晶界迁移的定量分析

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Diffusion induced grain boundary migration (DIGM) in the Cu(Zn) system was experimentally studied by Li and Hillert using polycrystalline Cu specimens zincified with binary Cu-Zn alloys containing 3.9-30.5 wt of Zn at temperatures between 573 and 773 K. Their experimental results have been quanti- tatively analyzed using the energy balance model proposed by Kajihara and Gust. The effective driving force Δ~efG for DIGM has been evaluated from the migration rate ν of the moving boundary and the com- position in the region alloyed with Zn behind the moving boundary, and then the mobility M of the mov- ing boundary has been calculated using the relationship M = ν/Δ~ef G. According to the analysis, the grain boundary migration obeys the chemical driving force model proposed by Hillert and Purdy for the largest experimental values of ν at 573 and 623 K. However, the chemical driving force is partially consumed by the volume diffusion of Zn in the Cu matrix ahead of the moving boundary for the other experimental values of ν at 623-773 K. In such a case, the migration rate dependence of the effective driving force should be taken into consideration. The temperature dependence of the mobility gives a value of QM = 177 kJ/mol as the activation enthalpy for the grain boundary migration. This value is close to the activation enthalpy for volume diffusion of Zn in Cu, 191 kJ/mol. Consequently, the grain boundary mi- gration is considered to be controlled by the solute drag effect due to the volume diffusion of Zn in the Cu matrix in the neighborhood of the moving boundary.
机译:Li和Hillert使用在573至773 K之间的温度下,用含3.9-30.5 wt%Zn的二元Cu-Zn合金镀锌的多晶Cu样品,对Cu(Zn)系统中的扩散诱导晶界迁移(DIGM)进行了实验研究。使用Kajihara和Gust提出的能量平衡模型对结果进行了定量分析。根据运动边界的迁移率ν和运动边界后面的与Zn合金化的区域中的成分,对DIGM的有效驱动力Δ〜efG进行了评估,然后得出了运动边界的迁移率M根据关系式M =ν/Δ〜ef G计算得出。对于分析在573和623 K时ν的最大实验值,晶界迁移服从Hillert和Purdy提出的化学驱动力模型。对于其他在623-773 K时的ν实验值,驱动力部分地被Zn在运动边界之前的Cu基体中的体积扩散所消耗。在这种情况下,应考虑有效驱动力的迁移率依赖性考虑在内。迁移率的温度依赖性给出QM = 177 kJ / mol的值作为晶界迁移的活化焓。该值接近于191 kJ / mol的Zn在Cu中的体积扩散的活化焓。因此,由于锌在移动边界附近在铜基体中的体积扩散,晶粒边界的迁移被认为是由溶质拖曳效应控制的。

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