Coefficients for the range, 839 to 1320C, were determined by using the residual activity method and 48V in alloys containing 0 to 90wt%V. Analysis of the results (table 203) showed that, at a given temperature, the variation in ln[D(C)] was linear in the concentration range of 1.6 to 28wt%V, and parabolic in V-rich solutions (65 to 90wt%V). In both cases, the diffusivity of V decreased with increasing V concentration. Peaks in the ln[Do(C)] and activation energy curves, found at 24wt%V, were attributed to the effect of the Fe3V ordered structure. Similar peaks, observed at 75wt%V, were similar to those noted in the Fe-Cr system.
K.Obrtlik, J.Kucera: Physica Status Solidi A, 1979, 53[2], 589-98
Table 204
Diffusion of C in Fe-1.1at%W at 1000C
C (at%) | D (cm2/s) |
0.6 | 1.1 x 10-7 |
1.1 | 1.2 x 10-7 |
2.2 | 1.25 x 10-7 |
Table 205
Diffusion Parameters for Zn in α-Fe
Zn (at%) | Do (cm2/s) | E (kJ/mol) |
0 | 60 | 262.6 |
2 | 38 | 256.2 |
4 | 19 | 247.5 |
6 | 11 | 239.9 |
8 | 6.2 | 232.9 |
10 | 3.9 | 226.4 |
12 | 2.0 | 218.1 |