The tracer diffusion of 181Hf, 95Nb and 95Zr was measured in the body-centered cubic structures of Hf-Nb alloys in order to determine whether the Arrhenius plot for self-diffusion exhibited any curvature; as in the case of body-centered cubic Zr-Nb alloys. In the case of the latter alloys, a continuous change in the diffusion anomaly with respect to self-diffusion in pure body-centered cubic Zr had been found. This reflected the systematic variation in electronic structure which occurred upon alloying group-V with group-VI body-centered cubic transition metals. The classification of self-diffusion in body-centered cubic Hf as normal or anomalous had not been possible because of its existence range of only 485K. The alloying of Hf with Nb stabilized the body-centered cubic structure to lower temperatures and considerably extended its existence range. Because the phonon-related diffusion model predicted self-diffusion in body-centered cubic Hf to lead to curved Arrhenius plots, it was expected that such curvature would be exhibited by the Hf-Nb alloys. However, measurements (tables 118 to 125) yielded straight plots for the present alloys.
P.Knorr, C.Herzig: Journal of Physics - Condensed Matter, 1995, 7[48], 9185-200
Table 119
Diffusivity of 95Nb in Hf-18at%Nb
Temperature (K) | D (m2/s) |
1257 | 7.97 x 10-16 |
1319 | 3.18 x 10-15 |
1529 | 6.62 x 10-14 |
1633 | 1.04 x 10-13 |
1981 | 3.05 x 10-12 |
2173 | 1.33 x 10-11 |
Table 120
Diffusivity of 181Hf in Hf-10at%Nb
Temperature (K) | D (m2/s) |
1758 | 9.36 x 10-13 |
1863 | 2.16 x 10-12 |
2003 | 4.63 x 10-12 |
2113 | 8.68 x 10-12 |
2268 | 1.78 x 10-11 |