| 研究生: |
何念葶 He, Nien-Ting |
|---|---|
| 論文名稱: |
Sn-xCu系及Sn-0.4Cu-0.3Ni無鉛銲錫合金振動破壞特性之微觀組織效應 Effects of Microstructure on the Vibration Fracture Characteristics of Sn-xCu and Sn-0.4Cu-0.3Ni Lead-Free Solder Alloys |
| 指導教授: |
陳立輝
Chen, Li-Hui 呂傳盛 Lui, Truan-Sheng |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 材料科學及工程學系 Department of Materials Science and Engineering |
| 論文出版年: | 2006 |
| 畢業學年度: | 94 |
| 語文別: | 中文 |
| 論文頁數: | 67 |
| 中文關鍵詞: | 無鉛銲錫 、振動 |
| 外文關鍵詞: | Sn-Cu, lead-free solder |
| 相關次數: | 點閱:153 下載:1 |
| 分享至: |
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銲錫材料可能被使用於振動的環境而造成損害,因此銲錫材料之振動特性有其探討的必要。本研究為探討微觀組織對Sn-xCu(x=0.3, 0.6, 1.3, 1.7wt.%)與Sn-0.4Cu-0.3Ni之振動特性之影響,並與Sn-Pb比較。
Sn-xCu系合金的微觀組織為樹枝狀初晶β-Sn與散佈的第二相Cu6Sn5。0.3Cu、0.6Cu和1.3Cu有粗大的樹枝狀β-Sn及共晶組織,1.3Cu另有較粗大的棒狀Cu6Sn5,而1.7Cu則整體微細化,包含β-Sn與Cu6Sn5皆較前三者細小。Sn-0.4Cu-0.3Ni的微觀組織包含β-Sn與Cu6Sn5外,還有粗大的Ni-Sn 化合物及微細的Sn-Cu-Ni 化合物散佈。在Sn-37Pb方面,為連續的第二相富鉛相分佈在Sn基地上。
由相近初始偏移量之共振壽命,可知各組材料之裂縫傳播阻抗能力之優劣,其中以0.3Cu最佳,0.3Ni最差。由等出力值的D-N曲線初始偏移量,可知各組材料之制振性,其中以0.3Cu最佳,37Pb最差。在等出力值條件下,各組材料之共振壽命由高至低依序為:0.6Cu>0.3Cu>0.3Ni>1.7Cu>1.3Cu>37Pb。
Sn-xCu系合金與Sn-0.4Cu-0.3Ni裂縫起始位置皆為層狀變形,裂縫也是沿著層狀變形傳播,而IMC會對裂縫傳播成阻礙;在Sn-37Pb中,裂縫起始位置則是在富錫相之晶界,而裂縫為沿著富錫相之晶界及富錫相與富鉛相之界面傳播。故在Sn-xCu系及Sn-0.4Cu-0.3Ni合金中,振動變形機制由層狀變形主導;Sn-37Pb合金之振動變形機制則由層狀變形與富錫相之晶界及富錫相與富鉛相之界面所主導。
The solder may be damaged under the circumstances of mechanical vibration, particularly when the vibrational frequency approaches the resonant frequency of the structure. So it is worthwhile to know the vibration-fracture resistance of the solder during alloy design. The effect of microstructure on the vibration fracture properties is investigated in this study. The aim of this study is to explore the deformation structure and the vibration fracture properties of Sn-xCu (x=0.3, 0.6, 1.3, 1.7wt.%) and Sn-o.4Cu-0.3Ni lead-free solder alloys. A comparison with the traditional Sn-37Pb solder will also be shown in the following.
The microstructure of the Sn-xCu alloys is composed of the dendritic primary phase β-Sn and the discretely distributed second phase Cu6Sn5. Large dendritic β-Sn is found in Sn-0.3Cu, Sn-0.6Cu and Sn-1.3Cu. The thick bar-shaped Cu6Sn5 is also found in the Sn-1.3Cu. However, the overall microstructure of Sn-1.7Cu become finer during the process, and both the primary phase and the second phase of Sn-1.7Cu are finer than the others. Besides β-Sn and Cu6Sn5, the Ni-Sn compounds and the Sn-Cu-Ni compounds are also found in the Sn-0.4Cu-0.3Ni. The Pb-rich phase is continuously distributed within the Sn-rich matrix of the Sn-37Pb solder.
Under the condition of constant initial deflection, the better vibration life is related to the better vibration fracture resistance. The result of vibration test performed under the condition of constant initial deflection indicates that the resistance of the Sn-0.3Cu is the best and that of the Sn-37Pb is the worst.
Under the condition of constant-force, the solder with a higher damping capacity possesses lower initial deflection amplitude. For the results, the damping capacity of the Sn-0.3Cu is the best and that of the Sn-0.4Cu-0.3Ni is the worst. Thus, under the condition of constant force, the specimen’s vibration life in descending order is: Sn-0.6Cu, Sn-0.3Cu, Sn-0.4Cu-0.3Ni, Sn-1.7Cu, and Sn-1.3Cu to Sn-37Pb.
A layer-like deformation appears at the outset of crack of the Sn-xCu and Sn-0.4Cu-0.3Ni alloys, and the crack propagates along the layer-like deformation. However, the intermetallic compound would impede the crack’s propagation. The vibration crack in the Sn-37Pb solder begins at the grain boundary of rich-Sn phase, and it propagates along the interphase of Sn/Pb grain boundaries and the Sn/Sn grain boundaries. Therefore, in the Sn-xCu and Sn-0.4Cu-0.3Ni lead-free solders, the layer-like deformation dominates the mechanism of vibration deformation. In the Sn-37Pb, the vibration deformation mechanism is dominated by the layer-like deformation, the Sn/Pb interphase boundaries and the Sn/Sn grain boundaries.
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