The pressure dependence of self-diffusion in the high-temperature body-centered cubic phase of Zr was studied by using radio-tracer techniques. Activation volumes of 0.184Ω at 1423K and 0.213Ω at 1273K were obtained, where Ω was the atomic volume. The activation volumes for 95Nb diffusion were equal to 0.161Ω at 1423K and 0.193Ω at 1273K. The small activation volumes indicated a large relaxation of the vacancy. This in turn reflected the inherent weakness, of the body-centered cubic lattice, with regard to shear in the <111> direction. These results (table 348) provided an explanation for the absence of positron trapping in group-IV transition metals.
P.Knorr, J.Jun, W.Lojkowski, C.Herzig: Physical Review B, 1998, 57[1], 334-40
Table 347
Diffusion of 95Zr in Zr
Temperature (K) | D (m2/s) |
1200 | 9.20 x 10-14 |
1250 | 1.26 x 10-13 |
1282 | 1.55 x 10-13 |
1333 | 2.16 x 10-13 |
1385 | 2.99 x 10-13 |
1424 | 3.76 x 10-13 |
1455 | 4.84 x 10-13 |
1478 | 5.05 x 10-13 |
1501 | 6.30 x 10-13 |
1518 | 8.05 x 10-13 |