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