The pressure dependence of diffusion in the high-temperature body-centered cubic phase of Zr was studied by using radio-tracer techniques. The activation volumes for 95Nb diffusion were equal to 0.161 Ω at 1423K and 0.193 Ω 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 279) 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 278

Diffusion of Hf in Polycrystalline Ultra-Pure or Fe-Doped -Zr

 

Sample

Temperature (K)

D (m2/s)

ultra-pure

1111.0

1.1 x 10-19

Fe-doped

1110.9

1.1 x 10-17

ultra-pure

1052.6

7.6 x 10-20

ultra-pure

1000.0

8.2 x 10-21

ultra-pure

934.2

5.3 x 10-22

Fe-doped

933.4

1.1 x 10-18

ultra-pure

873.0

2.5 x 10-23