The pressure dependence of the diffusivity of transition elements (table 25) was studied by using the radio-tracer method, with serial sectioning by microtome. The radio-isotopes were implanted so as to avoid problems with oxide hold-up and with the low solubility of transition elements. Diffusion annealing was then carried out in a high-pressure cell at Ar pressures of up to 0.8GPa. The activation volumes for diffusion were determined by isothermal annealing. It was recalled that the activation volumes of non-transition elements were close to one atomic volume, and were not very different from the activation volume for self-diffusion. On the other hand, the transition elements had diffusion activation volumes of between 2.7 and 1.67 atomic volumes. They were also characterized by high activation enthalpies and pre-exponential factors. The results were explained in terms of differences, in vacancy-solute interaction, between transition and non-transition solutes. The results could be described by:
D (m2/s) = 7.7 x 10-1 exp[-221(kJ/mol)/RT]
G.Rummel, T.Zumkley, M.Eggersmann, K.Freitag, H.Mehrer: Zeitschrift für Metallkunde, 1995, 86[2], 131-40
Table 25
Diffusivity of 59Fe in Al under Hydrostatic Pressure
Temperature (K) | Pressure (MPa) | D (m2/s) |
854 | 37 | 1.90 x 10-16 |
854 | 172 | 1.34 x 10-16 |
854 | 286 | 9.08 x 10-15 |
854 | 310 | 8.52 x 10-15 |
854 | 437 | 5.52 x 10-15 |
854 | 642 | 2.50 x 10-15 |
894 | 6 | 7.03 x 10-16 |
894 | 181 | 3.44 x 10-16 |
894 | 356 | 1.85 x 10-16 |
894 | 520 | 1.17 x 10-16 |
894 | 673 | 5.76 x 10-15 |