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