It was shown that that the diffusivity was different when measured during or after cathodic charging. The diffusivities at 25C were equal to 3 x 10-6cm2/s during charging and 3.4 x 10-7cm2/s after charging. The overall results could be described by:
during charging: D (cm2/s) = 1.48 x 10-4 exp[-0.1(eV)/kT]
after charging: D (cm2/s) = 3.11 x 10-4 exp[-0.175(eV)/kT]
They were explained in terms of 2 different types of H trapping; one type being reversible (during charging) and the other being irreversible (de-gassing after charging).
H.Veysseyre: Met. Corros. Ind., 1966, 495, 405-24
Table 56
Diffusivity of H in Fe at 20C as a Function of Rolling Deformation
Deformation (%) | D (cm2/s) | Trap Density (/cm3) | Dislocation Density (/cm2) |
8.8 | 5.1 x 10-5 | 5.7 x 1018 | 5.6 x 109 |
20 | 5.5 x 10-5 | 4.5 x 1018 | 8.6 x 109 |
22 | 5.1 x 10-5 | 5.7 x 1018 | 9.1 x 109 |
28 | 4.3 x 10-5 | 8.5 x 1018 | 1.07 x 1010 |
30 | 4.4 x 10-5 | 8.1 x 1018 | 1.13 x 1010 |
41 | 4.4 x 10-5 | 8.1 x 1018 | 1.42 x 1010 |
51 | 4.1 x 10-5 | 9.4 x 1018 | 1.68 x 1010 |
60 | 4 x 10-5 | 9.9 x 1018 | 1.92 x 1010 |