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