The tracer diffusion of H in body-centered cubic TiHx phases, with x = 0.57 or 0.70, was measured at temperatures ranging from 620 to 830K by using the nuclear magnetic resonance pulsed field gradient spin-echo technique. It was found that the results could be described by the expressions:
x = 0.57: D (cm2/s) = 7.8 x 10-4 exp[-0.155(eV/atom)/kT]
x = 0.70: D (cm2/s) = 6.3 x 10-4 exp[-0.147(eV/atom)/kT]
The diffusion parameters were compared with those for other body-centered cubic transition metal hydrides. All were found to have large H-diffusion coefficients, which decreased as the H concentration was increased. Although an increase in H concentration caused an increase in activation energy over most of the concentration range, the maximum value of the activation energy did not exceed 0.190eV/atom. In contrast, it was noted that most face-centered cubic transition metal hydrides had activation energies which were higher, by a factor of 3 or more, and diffusion coefficients which were smaller by 2 or more orders of magnitude.
Tracer Diffusion Coefficients of Hydrogen at High Concentration in BCC Host Metal Lattices. E.H.Sevilla, R.M.Cotts: Journal of the Less-Common Metals, 1987, 129, 223-8
Table 169
Diffusion of H in Ti and Ti-V Alloys
Material | Temperature (C) | Do (cm2/s) | E (eV) |
TiH0.70 | 282-352 | 6.4 x 10-4 | 0.147 |
TiH0.57 | 390-416 | 7.8 x 10-4 | 0.150 |
Ti0.96V0.04H0.70 | 180-352 | 3.7 x 10-4 | 0.115 |
Ti0.96V0.04H0.54 | 253-333 | 4.5 x 10-4 | 0.124 |
Ti0.96V0.04H0.39 | 393-496 | 4.9 x 10-4 | 0.130 |
Ti0.92V0.08H0.41 | 282-372 | 6.0 x 10-4 | 0.140 |