The diffusivity and solubility of H in grain-refined material were measured by using a vacuum hot-extraction method. Four samples, with various grain sizes, were prepared by melting, adding Ti and B, casting, re-melting and solidifying unidirectionally. The grain-refined samples contained small particles within the matrix. It was found that the H diffusivity obeyed an Arrhenius type behavior at temperatures ranging from 573 to 873K. The results for air-melted Al-0.05wt%Ti samples could be described by:
D (m2/s) = 2.04 x 10-4exp[-65.7(kJ/mol)/RT]
and the results for Al-0.05wt%Ti samples which had been cast under flowing N could be described by:
D (m2/s) = 2.22 x 10-6exp[-37.4(kJ/mol)/RT]
The equivalent relationships for Al-0.1wt%Ti samples could be described by:
D (m2/s) = 9.10 x 10-3exp[-95.4(kJ/mol)/RT]
D (m2/s) = 1.39 x 10-4exp[-66.9(kJ/mol)/RT]
respectively. The diffusivity was not affected by the small particles in the matrix, and depended only upon the grain size. A so-called grain-boundary cross effect, which referred to fast diffusion along grain boundaries and suppressed diffusion due to H trapping at nodes or grain boundary junctions, was confirmed. A linear relationship, the so-called compensation effect, was found between the logarithm of the pre-exponential factor and the activation energy for all of the materials which were studied here.
Diffusivity and Solubility of Hydrogen in Grain-Refined Aluminum. M.Ichimura, Y.Sasajima: Materials Transactions, 1993, 34[5], 404-9
Table 5
Diffusion Parameters for H in Al
Grain Size (mm) | Voids (vol%) | T (K) | Do(m2/s) | Q (kJ/mol) |
monocrystal | 0 | 473-903 | 9.53 x 10-6 | 44.3 |
15 | 0 | 573-923 | 4.58 x 10-6 | 37.0 |
4 | 0 | 573-903 | 1.52 x 10-5 | 53.4 |
2 | 0.04 | 623-913 | 2.11 x 10-4 | 67.0 |
3 | 0.17 | 623-903 | 1.54 x 10-3 | 81.2 |
3 | 0.50 | 623-903 | 4.22 x 10-2 | 106.9 |
4 | 0.19 | 573-903 | 6.00 x 10-3 | 88.7 |