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 0.161Ω 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 343) 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 343

Diffusivity of 95Nb in β-Zr

 

Temperature (K)

Pressure (MPa)

D (m2/s)

1273

110

4.438 x 10-14

1273

303

4.317 x 10-14

1273

601

3.957 x 10-14

1273

904

3.793 x 10-14

1273

1110

3.672 x 10-14

1273

1300

3.147 x 10-14

1423

103

1.732 x 10-13

1423

303

1.576 x 10-13

1423

605

1.534 x 10-13

1423

903

1.467 x 10-13

1423

1101

1.373 x 10-13

1423

1301

1.360 x 10-13