Solidification microstructures in Ag3Sn-Cu3Sn pseudo …€¦ ·  · 2016-06-23Title: Microsoft...

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Solidification Microstructures in Ag 3 Sn-Cu 3 Sn Pseudo-Binary Alloys H. Yu, Y. Sun, S. P. Alpay and M. Aindow Department of Materials Science and Engineering, Institute of Materials Science, University of Connecticut, Unit 3136, 97 North Eagleville Road, Storrs, CT 06269-3136, USA The intermetallic phases θ-Ag 3 Sn and ε 1 -Cu 3 Sn are common constituents in Sn-rich ternary Ag-Cu-Sn alloy systems, which are good candidates for Pb-free solders [1]. Both can be present as minority strengthening phases in the solder alloy and can form as reaction products at solder/substrate interfaces [2]. Studying the properties of these phases is challenging because the phase equilibria make the production of good quality single-phase samples very difficult. In binary systems, θ-Ag 3 Sn forms via a sluggish peritectic reaction between Sn-rich liquid and ε 2 -Ag 5 Sn [3], while ε 1 -Cu 3 Sn forms via congruent ordering from γ-Cu 4 Sn, which is itself a peritectic reaction product [4]. In the present study, we selected three alloys with Ag 3 Sn-Cu 3 Sn pseudo-binary compositions and examined the solidification microstructures to evaluate the extent to which the complex phase equilibria can be avoided. Three (Ag,Cu) 3 Sn alloys having Ag:Cu ratios of 50:50, 40:60 and 30:70 were selected for this study. Backscattered electron (BSE) SEM images and energy-dispersive X-ray spectroscopy (EDXS) data were obtained from the polished sample surfaces in a FEI Teneo LoVac SEM. Small pieces of alloy samples with an approximate weight of 10 mg were used for differential scanning calorimetry (DSC) analyses. The initial analyses were performed in a TA Instruments SDT Q600 under a purified argon atmosphere using a heating rate of 10 °C/min. Parallel heating and quenching experiments were performed in a TA Instruments DSC 2920, which allows for the rapid removal of samples from the apparatus, under the same atmosphere environment and heating rate. The microstructures of the quenched samples were examined on the metallographic sections using BSE imaging and EDXS analyses in the SEM. The as-cast microstructures (Fig. 1) contain mainly the θ-Ag 3 Sn (light region) and ε 1 -Cu 3 Sn (dark region) with a little η-Cu 6 Sn 5 (gray region). There is no evidence for the presence of high-temperature phases or segregation, which is not what one would expect on the basis of the published ternary phase diagram. The following DSC and heat-treatment/quenching studies were performed to investigate these phenomena. The DSC data (Fig. 2) revealed three invariant processes: at 355 °C, η à ε 1 + L; at 482 °C, θ à ε 2 + L; and at 531 °C, ε 1 + ε 2 à L. A composition-dependent fourth process corresponds to melting of primary ε 1 -Cu 3 Sn. While the transformations that occur upon heating are consistent with the previous studies, most of the solidification microstructures do not follow the expectations on this basis. BSE SEM images from the quenched 50:50, 40:60 and 30:70 alloys (Figs. 3 & 4) revealed: Samples quenched from 400 °C contained θ and ε 1 grains but no η phase (Fig. 3a); Samples quenched from 500 °C contained coarse θ and ε 1 grains plus a complex phase mixture of ε 1 , ε 2 , η, and β-Sn (Figs 3b, 4a & 4b); Samples quenched from 545 °C contained coarse angular ε 1 grains plus a fine eutectic mixture of θ and ε 1 (Figs. 3c, 4c & 4d); Samples quenched from 600 °C exhibited more diverse microstructures. The 50:50 alloy sample contained fine ε 1 grains plus a eutectic mixture of θ and ε 1 (Fig. 3d). The 40:60 alloy sample contained fine feathery ε 1 grains with interdendritic θ, η, and β grains (Fig. 4e). The 30:70 alloy sample contained coarse ε 1 grains plus a refined version of the phase mixture in the 40:60 alloy sample (Fig. 4f). It is proposed that the solidification microstructures must correspond to the nucleation of the high- temperature phases being kinetically limited upon cooling for these compositions, which leads to the direct formation of the equilibrium low-temperature phases by eutectic-type co-operative growth [5]. [6]

Transcript of Solidification microstructures in Ag3Sn-Cu3Sn pseudo …€¦ ·  · 2016-06-23Title: Microsoft...

Page 1: Solidification microstructures in Ag3Sn-Cu3Sn pseudo …€¦ ·  · 2016-06-23Title: Microsoft Word - Solidification microstructures in Ag3Sn-Cu3Sn pseudo-binary alloys - Aindow

Solidification Microstructures in Ag3Sn-Cu3Sn Pseudo-Binary Alloys H. Yu, Y. Sun, S. P. Alpay and M. Aindow Department of Materials Science and Engineering, Institute of Materials Science, University of Connecticut, Unit 3136, 97 North Eagleville Road, Storrs, CT 06269-3136, USA The intermetallic phases θ-Ag3Sn and ε1-Cu3Sn are common constituents in Sn-rich ternary Ag-Cu-Sn alloy systems, which are good candidates for Pb-free solders [1]. Both can be present as minority strengthening phases in the solder alloy and can form as reaction products at solder/substrate interfaces [2]. Studying the properties of these phases is challenging because the phase equilibria make the production of good quality single-phase samples very difficult. In binary systems, θ-Ag3Sn forms via a sluggish peritectic reaction between Sn-rich liquid and ε2-Ag5Sn [3], while ε1-Cu3Sn forms via congruent ordering from γ-Cu4Sn, which is itself a peritectic reaction product [4]. In the present study, we selected three alloys with Ag3Sn-Cu3Sn pseudo-binary compositions and examined the solidification microstructures to evaluate the extent to which the complex phase equilibria can be avoided. Three (Ag,Cu)3Sn alloys having Ag:Cu ratios of 50:50, 40:60 and 30:70 were selected for this study. Backscattered electron (BSE) SEM images and energy-dispersive X-ray spectroscopy (EDXS) data were obtained from the polished sample surfaces in a FEI Teneo LoVac SEM. Small pieces of alloy samples with an approximate weight of 10 mg were used for differential scanning calorimetry (DSC) analyses. The initial analyses were performed in a TA Instruments SDT Q600 under a purified argon atmosphere using a heating rate of 10 °C/min. Parallel heating and quenching experiments were performed in a TA Instruments DSC 2920, which allows for the rapid removal of samples from the apparatus, under the same atmosphere environment and heating rate. The microstructures of the quenched samples were examined on the metallographic sections using BSE imaging and EDXS analyses in the SEM. The as-cast microstructures (Fig. 1) contain mainly the θ-Ag3Sn (light region) and ε1-Cu3Sn (dark region) with a little η-Cu6Sn5 (gray region). There is no evidence for the presence of high-temperature phases or segregation, which is not what one would expect on the basis of the published ternary phase diagram. The following DSC and heat-treatment/quenching studies were performed to investigate these phenomena. The DSC data (Fig. 2) revealed three invariant processes: at 355 °C, η à ε1 + L; at 482 °C, θ à ε2 + L; and at 531 °C, ε1 + ε2 à L. A composition-dependent fourth process corresponds to melting of primary ε1-Cu3Sn. While the transformations that occur upon heating are consistent with the previous studies, most of the solidification microstructures do not follow the expectations on this basis. BSE SEM images from the quenched 50:50, 40:60 and 30:70 alloys (Figs. 3 & 4) revealed: Samples quenched from 400 °C contained θ and ε1 grains but no η phase (Fig. 3a); Samples quenched from 500 °C contained coarse θ and ε1 grains plus a complex phase mixture of ε1, ε2, η, and β-Sn (Figs 3b, 4a & 4b); Samples quenched from 545 °C contained coarse angular ε1 grains plus a fine eutectic mixture of θ and ε1 (Figs. 3c, 4c & 4d); Samples quenched from 600 °C exhibited more diverse microstructures. The 50:50 alloy sample contained fine ε1 grains plus a eutectic mixture of θ and ε1 (Fig. 3d). The 40:60 alloy sample contained fine feathery ε1 grains with interdendritic θ, η, and β grains (Fig. 4e). The 30:70 alloy sample contained coarse ε1 grains plus a refined version of the phase mixture in the 40:60 alloy sample (Fig. 4f). It is proposed that the solidification microstructures must correspond to the nucleation of the high-temperature phases being kinetically limited upon cooling for these compositions, which leads to the direct formation of the equilibrium low-temperature phases by eutectic-type co-operative growth [5]. [6]

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References: [1] M Abtew and G Selvaduray, Mater. Sci. Eng. R 27 (2000) 95. [2] CM Hsu and SW Chen, J. Mater. Sci. 48 (2013) 6640. [3] I Karakaya and WT Thompson, Bull. Alloy Phase Diagr. 8 (1987) 340. [4] N Saunders and AP Miodownik, Bull. Alloy Phase Diagr. 11 (1990) 278. [5] H Yu, Y Sun, SP Alpay and M Aindow, J Mater Sci 51 (2016) 6474. [6] The microscopy studies were performed in the UConn/FEI Center for Advanced Microscopy and Materials Analysis (CAMMA).

Figure 1. Representative BSE SEM images obtained from as-cast samples of the alloys: a) 50:50; b) 40:60; c) 30:70.

Figure 2. Plots of DSC heat flow data obtained from as-cast alloy samples at a heating rate of 10 °C/min.

Figure 3. Representative BSE SEM images obtained from 50:50 alloy samples quenched to room temperature from: a) 400 °C; b) 500 °C; c) 545 °C; d) 600 °C.

Figure 4. Representative BSE SEM images obtained from the 40:60 (a,c,e) and 30:70 alloy (b,d,f) samples quenched from: (a,b) 500 °C; (c,d) 545 °C; (e,f) 600 °C.