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首页> 外文期刊>Materials transactions >Kinetics of Static Grain Growth in Dynamically Recrystallized Copper Polycrystals with Different Purities
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Kinetics of Static Grain Growth in Dynamically Recrystallized Copper Polycrystals with Different Purities

机译:不同纯度的动态重结晶铜多晶中晶粒长大的动力学。

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Effect of purity on static softening and grain growth taking place after dynamic recrystallization (DRX) was studied by means of interrupted compression tests and metallographic observations of polycrystalline copper specimens with three different purities of 99.9 (3N), 99.99 (4N) and 99.9999 (6N) mass percent. The fractional softening-annealing time (X-t) curves after dynamic recovery consist of two stages, followed by complete softening. In contrast, the softening curves for DRX matrices consist of three distinct stages accompanied with three plateaus, followed by incomplete softening (stages I, II and III). The X-t curves for DRX matrices of specimens 3N and 4NCu are almost the same, but clearly different from that for specimen 6NCu. The static softening for a DRX matrix of specimen 6NCu takes place one order of magnitude faster than that for specimen 3N or 4NCu and finally approaches X= 1 after a long period of annealing time in stage III. The average rate of grain growth in stage III is always smaller than that for normal grain growth, although both the rates are controlled by grain boundary diffusion irrespective of purity of copper. This results from the stable existence of metadynamically recovered grains which have many-sided irregular shapes as well as high density dislocations. As these grains are metastable in thermodynamics, however, DRX matrices only for specimen 6NCu finally replace fully recrystallized ones, followed by the occurrence of normal grain growth.
机译:通过间断压缩试验和金相观察三种纯度分别为99.9(3N),99.99(4N)和99.9999(6N)的多晶铜试样,研究了纯度对动态重结晶(DRX)后发生的静态软化和晶粒生长的影响。 )质量百分比。动态恢复后的软化退火时间分数(X-t)曲线包括两个阶段,然后进行完全软化。相比之下,DRX矩阵的软化曲线包括三个不同的阶段以及三个平稳阶段,然后是不完全的软化(阶段I,II和III)。样品3N和4NCu的DRX矩阵的X-t曲线几乎相同,但与样品6NCu的X-t曲线几乎相同。样品6NCu的DRX矩阵的静态软化比样品3N或4NCu的静态软化快一个数量级,并且在阶段III中经过长时间的退火后,最终达到X = 1。第三阶段的平均晶粒生长速率始终小于正常晶粒生长的速率,尽管这两种速率均受晶界扩散的控制,而与铜的纯度无关。这是由于稳定地存在了动力学恢复的晶粒,该晶粒具有多面不规则形状以及高密度位错。由于这些晶粒在热力学上是亚稳态的,因此仅用于试样6NCu的DRX矩阵最终替代了完全重结晶的晶粒,随后出现正常的晶粒生长。

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