使用单搭接剪切试验表征无铅焊点

S. Pin, H. Frémont, A. Gracia
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引用次数: 3

摘要

该研究的目的是表征一种无铅焊料材料在代表性尺度上的机械行为。在这项工作中考虑的具体合金是SnAg0.3Cu0.5。试验台包括特定的单搭接剪切试样几何形状,具有与非接触监测方法相关的凹槽。这允许测试具有代表微电子应用厚度的焊点,在回流过程中具有良好的热梯度,因此具有与BGA尺寸相似的冶金性能。试验包括3种不同温度下的单调剪切试验和蠕变试验。本文强调了制造过程和监测数据处理,因为如果不采取预防措施,由于关节的规模缩小,它可能导致不一致的结果。一旦微观结构得到验证,实验数据就可以用来确定特定的粘塑性材料行为。事实上,初次蠕变应变对于常见的二次蠕变速率是显著的。如果只考虑原焊料的二次蠕变应变,则循环载荷下的一次蠕变应变积累可能导致未来预测计算中的估计误差。在本研究中,不同应力水平下的连续蠕变步骤突出了这一点。循环硬化也进行了研究,但与模拟这种特殊的塑性行为无关。在- 40、25和125°C单调载荷下,材料系数的最后一组提供了完整的蠕变行为,结合了初级和次级蠕变状态以及杨氏模量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Lead free solder joints characterisation using single lap shear tests
The study aims at characterizing the mechanical behaviour of a lead free solder material at a representative scale. The specific alloy considered in this work is SnAg0.3Cu0.5. The test bench comprises a specific single lap shear specimen geometry with grooves associated to a contactless method of monitoring. This allows to test solder joints with a thickness representative of microelectronics applications with good thermal gradients during the reflow process and thus metallurgic properties similar to the ones get with BGA dimensions. The campaign consists in monotonic shear tests and creep tests at 3 different temperatures. An emphasis on the fabrication process and the monitoring data treatment is given in this paper as it can leads to non-consistent results if not managed with precautions due to the reduced scale of the joint. Once the microstructure has been validated, experimental data are used to identify a specific viscoplastic material behaviour. Indeed, the primary creep strain has been found to be significant regarding the common secondary creep rate. Primary creep strain accumulation in cyclic loads could lead to an error of estimation in future predictive calculations if only secondary creep strain was considered as for the former solder materials. It is highlighted by successive creep steps at various stress levels performed in this study. Cyclic hardening has also been investigated but turns to be not relevant to model this particular plastic behaviour. The final set of material coefficients is provided for a full creep behaviour combining primary and secondary creep states coupled with Young's moduli at −40, 25 and 125°C monotonic loads.
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