The migration of H in high-purity material was studied by using the Gorsky-effect anelastic technique. The observed H diffusivities depended upon the concentrations of trapping sites such as dislocations and O atoms. At low interstitial solute levels and low dislocation densities (104/cm2), the activation energy was 0.080eV. As the number of O trapping sites increased, the activation energy increased to a value of 0.096eV at 0.23at%O (table 85). The introduction of dislocation trapping sites by cold-rolling (10% reduction of area) increased the activation energy to 0.093eV. High activation energies were also observed in specimens which contained high H concentrations after extensive hydride precipitation had occurred. This was consistent with the large amount of plastic deformation that occurred when such hydrides were precipitating.
G.Matusiewicz, R.Booker, J.Keiser, H.K.Birnbaum: Scripta Metallurgica, 1974, 8[12], 1419-25
Table 84
Parameters for H Diffusion in NbHx
x | Do (cm2/s) | E (eV) |
0.10 | 3.2 x 10-4 | 0.115 |
0.33 | 4.9 x 10-4 | 0.142 |
0.55 | 1.0 x 10-3 | 0.168 |
0.70 | 7.2 x 10-4 | 0.174 |
0.89 | 5.6 x 10-4 | 0.164 |
Figure 16
Diffusivity of H in Nb
Table 85
Parameters for H Diffusion in Nb at Temperatures above 165K
O (at%) | N (at%) | C (at%) | H (at%) | Method | Do (cm2/s) | E (eV) |
0.14 | 0.06 | <0.01 | 2.2 | dynamic | 2.8 x 10-4 | 0.089 |
0.08 | 0.02 | <0.01 | 1.6 | dynamic | 2.8 x 10-4 | 0.089 |
0.23 | 0.005 | 0.006 | 0.28 | static | 2.4 x 10-4 | 0.096 |
0.043 | 0.006 | 0.005 | 0.095 | static | 1.7 x 10-4 | 0.081 |
0.029 | 0.009 | 0.005 | 0.11 | static | 1.6 x 10-4 | 0.080 |