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Kinetics of Pb-rich phase particle coarsening in Sn-Pb solder under isothermal annealing-cooling rate dependence

机译:等温退火-冷却速率相关的Sn-Pb焊料中富Pb相颗粒粗化的动力学

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摘要

The coarsening behavior of the Pb-rich phase particles in 63Sn-37Pb (wt percent) solder was investigated following isothermal annealing treatments. Samples were exposed to cooling rates of 0.1, 1.0, 10, and 100 deg C/min. Annealing temperatures were 25, 55, 70, 85, and 100 deg C, and times were 2-100 days. The mean particle diameter decreased from 1.8 X 10~(-3) to 0.8 X 10~(-3) mm with increased cooling rate, indicating two solidification regimes: one for cooling rates <=l deg C/min and the other for cooling rates of >=10 deg C/min. The Pb-rich phase particles coarsened more quickly in samples made at the two fastest cooling rates. There was little Pb-rich phase particle coarsening at 25 and 55 deg C for all annealing times. Coarsening rate kinetics were examined specifically for the 10 and 100 deg C/min data using the expression A_t~n exp[-triangle open H/RT]. The values of n were 0.23 +-0.11 and 0.36 +- 0.13, respectively; n was not sensitive to annealing temperature. The corresponding ln values indicated that the coarsening mechanism changed from a fast diffusion to a bulk diffusion controlled process with a faster cooling rate. The apparent activation energy triangle open H ranged from 16+-8 to 41+- 8 kJ/mol; the values increased with cooling rate from 10 to 100 deg C/min. The triangle open H value was sensitive to annealing temperature only for the faster cooling rate of 100 deg C/min. Together, the n and triangle open H values indicated that an accelerated, fast diffusion mechanism with low activation barriers characterized the Pb-rich phase coarsening in samples exposed to a slower cooling rate, greater annealing, or a combination of the two conditions. That mechanism likely originated from the in situ development of recover/recrystallization microstructures in the Sn-rich phase. At faster cooling rates, those microstructures were not as well developed, so coarsening was controlled more by the higher activation barriers of bulk diffusion processes.
机译:经过等温退火处理后,研究了63Sn-37Pb(wt%)焊料中富Pb相颗粒的粗化行为。样品暴露于0.1、1.0、10和100℃/ min的冷却速率下。退火温度为25、55、70、85和100摄氏度,时间为2-100天。随着冷却速率的增加,平均粒径从1.8 X 10〜(-3)毫米减小到0.8 X 10〜(-3)mm,表明两种固化方式:一种用于冷却速度<= 1℃/ min,另一种用于冷却速率> = 10摄氏度/分钟。在以最快的两个冷却速率制备的样品中,富铅相颗粒的粗化速度更快。在所有退火时间中,在25和55摄氏度下几乎没有富Pb的相颗粒粗化。使用表达式A_t〜n exp [-三角形开放H / RT],专门针对10和100℃/ min的数据检查了粗化速率动力学。 n的值分别为0.23±0.11和0.36±0.13。 n对退火温度不敏感。相应的ln值表明,粗化机理从快速扩散变为具有更快冷却速率的体扩散控制过程。表观活化能三角形开度H在16 + -8至41 + -8kJ / mol的范围内。冷却速度从10摄氏度/分钟增加到100摄氏度/分钟。三角形开度H值仅对于更快的100℃/ min的冷却速率对退火温度敏感。 n和三角形开放H值一起表明,具有低活化能垒的加速,快速扩散机制表征了暴露于较慢的冷却速率,更大的退火或两种条件的组合下的样品中富Pb的相粗化。该机制可能源自富锡相中恢复/再结晶微结构的原位形成。在较快的冷却速率下,那些微结构没有得到很好的发展,因此通过体扩散过程中较高的活化势垒来更多地控制粗化。

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