The diffusion coefficients were measured at temperatures ranging from 489 to 774K. The 16O was injected via ion implantation. The diffusion penetration profiles were then measured by exploiting the 16O(d,p)17*O nuclear reaction. The temperature dependence of the O diffusivity was described by:
D (m2/s) = 1.3 x 10-6 exp[-121.6(kJ/mol)/RT]
It was found that the addition of Si and Al hardly affected O diffusion, whereas the addition of Fe, Nb or B decreased the diffusivity by 20 to 70%, and the addition of Cr or Mo decreased the activation energy by 10 to 15% (table 315). The most marked alloying effect was observed in the case of the V-3Ti-2Si and V-5Ti alloys. The diffusivity in V-5Ti was about 2 orders of magnitude lower than that in V. It was concluded that this was evidence for a trapping effect due to Ti, and the binding energy was estimated to be about 52kJ/mol.
H.Nakajima, S.Nagata, H.Matsui, S.Yamaguchi: Philosophical Magazine A, 1993, 67[3], 557-71
Table 318
Diffusivity of 16O in V Alloys
Material | Temperature (K) | D (m2/s) |
V-0.1Al | 673 | 6.77 x 10-16 |
V-0.1Al | 623 | 9.30 x 10-17 |
V-0.1Al | 574 | 8.65 x 10-18 |
V-0.1Al | 532 | 1.44 x 10-18 |
V-0.1Al | 494 | 1.13 x 10-19 |
V-0.1B | 624 | 6.70 x 10-17 |
V-0.1B | 574 | 8.50 x 10-18 |
V-0.1B | 524 | 6.04 x 10-19 |
Table 319
Diffusion Coefficients for 60Co in V-Co Alloys
Co(at%) | Temperature(K) | D (m2/s) |
0 | 1521 | 6.20 x 10-15 |
0 | 1438 | 1.87 x 10-15 |
0 | 1403 | 9.3 x 10-16 |
0 | 1337 | 2.6 x 10-16 |
0.5 | 1521 | 7.95 x 10-15 |
0.5 | 1438 | 1.99 x 10-15 |
0.5 | 1403 | 1.10 x 10-15 |
0.5 | 1337 | 3.3 x 10-16 |
1.0 | 1521 | 8.49 x 10-15 |
1.0 | 1438 | 2.37 x 10-15 |
1.0 | 1403 | 1.14 x 10-15 |
1.0 | 1337 | 4.1 x 10-16 |
1.5 | 1521 | 1.03 x 10-14 |
1.5 | 1438 | 2.60 x 10-15 |
1.5 | 1403 | 1.89 x 10-15 |
1.5 | 1337 | 5.6 x 10-16 |
2.0 | 1521 | 1.24 x 10-14 |
2.0 | 1438 | 3.07 x 10-15 |
2.0 | 1403 | 2.55 x 10-15 |
2.0 | 1337 | 1.01 x 10-15 |