Alloys which contained up to 8at%Si were studied at 900 to 1150K by using semi-infinite couples and Kirkendall markers (table 104). The tracer diffusivity of Cu in pure Cu, and in alloys which contained up to 1.8at%Si, was also studied at 1130K by using the serial sectioning method. It was found that a non-linear enhancement of Cu diffusivity was caused by adding Si. The first- and second-order enhancement factors for solvent diffusivity were deduced to be 19.4 and 188, respectively. The Gibbs free energy of binding between a vacancy and a Si atom was estimated to be -11.8kJ/mol at 1130K. By using self-diffusivity data for pure Cu, and by extrapolating diffusion data on Cu-Si alloys to infinite dilution, the vacancy flow factor in the Cu-Si system at 1130K was deduced to be -0.62. Overall, the results indicated that there was a weak interaction between a vacancy and a Si atom in Cu.
Y.Iijima, Y.Wakabayashi, T.Itoga, K.Hirano: Materials Transactions A, 1991, 32[5], 457-64
Table 105
Interdiffusion Parameters for Cu-Si Alloys
Si (at%) | Do (m2/s) | E (kJ/mol) |
0 | 2.1 x 10-5 | 187 |
2.0 | 2.7 x 10-5 | 186 |
3.0 | 2.4 x 10-5 | 184 |
4.0 | 3.4 x 10-5 | 183 |
5.0 | 3.6 x 10-5 | 182 |
6.0 | 2.8 x 10-5 | 181 |
7.0 | 1.9 x 10-5 | 172 |
8.0 | 2.0 x 10-5 | 170 |
9.8 | 1.3 x 10-5 | 163 |
Table 106
Diffusion of 64Cu in Cu-15at%Sn
Temperature (K) | D(m2/s) |
1021.6 | 3.15 x 10-11 |
1020.4 | 2.56 x 10-11 |
1014.3 | 2.04 x 10-11 |
1000.4 | 2.00 x 10-11 |
988.7 | 2.02 x 10-11 |
986.6 | 1.57 x 10-11 |
951.0 | 1.21 x 10-11 |
931.6 | 9.06 x 10-12 |
907.7 | 7.78 x 10-12 |
883.6 | 6.01 x 10-12 |