Solute diffusion of these Al-substituting elements was investigated in Ni3Al single crystals with the composition Ni75.9Al24.1 over a wide temperature range (figure 11, table 15). The concentration profiles were determined by secondary ion mass spectrometry. The experimental data were analyzed in order to establish the governing diffusion mechanism. A model for the minority component diffusion by anti-structure defects had been suggested for the L12 structure. It involved both nearest-neighbor jumps of the solute atoms on the Ni sub-lattice as anti-structure atoms and the formation of so-called anti-structure bridges which corresponded to jumps between different sub-lattices. The model under consideration was shown to agree with the experimental data on the Al-substituting solute diffusion (X = Ga, Ge, Ti, Nb) in Ni3Al and permitted the observed ratio of the diffusivities DNi/Dx to be explained. These could be higher or lower than unity, depending upon the solute and temperature.
Solute Diffusion of Al-Substituting Elements in Ni3Al and the Diffusion Mechanism of the Minority Component. Divinski, S.V., Frank, S.T., Södervall, U., Herzig, C.: Acta Materialia, 1998, 46[12], 4369-80
Table 14
Grain boundary diffusivity of 67Ga in Ni3Al
Al(at%) | Temperature (K) | P(m3/s) |
24.8 | 1173 | 2.6 x 10-20 |
24.8 | 1073 | 6.6 x 10-21 |
24.8 | 973 | 3.6 x 10-22 |
24.8 | 873 | 3.0 x 10-23 |
24.8 | 773 | 1.2 x 10-24 |
23.8 | 1173 | 5.6 x 10-20 |
23.8 | 1073 | 8.6 x 10-21 |
23.8 | 973 | 7.1 x 10-22 |
23.8 | 873 | 4.8 x 10-23 |
23.8 | 773 | 1.6 x 10-24 |
22.4 | 1173 | 9.5 x 10-20 |
22.4 | 1073 | 1.9 x 10-20 |
22.4 | 973 | 2.3 x 10-21 |
22.4 | 873 | 8.1 x 10-23 |
22.4 | 773 | 2.5 x 10-24 |