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