The knowledge of self-diffusion of various elements was important for understanding and elucidating the long-term dissolution of the nuclear waste glass. The self-diffusion coefficients of Na and Cs in P0798 (SiO2-14.2B2O3-5Al2O3-3Li2O-3CaO-3wt%ZnO) simulated nuclear waste glass were measured (tables 2 and 3) by an ion beam sputter-sectioning technique using the radioactive isotopes 22Na and 137Cs. The temperature dependence of the diffusion coefficients in each temperature range in P0798 glass below the glass transition temperature Tg could be expressed by the following equations:

428-574K:     DNa (m2/s) = 2.7 x 10-6 exp[-113(kJ/mol)/RT]

713-758K:     DCs (m2/s) = 7.1 x 10-5 exp[-241(kJ/mol)/RT]

The diffusion coefficient of 22Na was about ten orders of magnitude larger than that of 137Cs at 573K. The large difference in the diffusion coefficients was explained in terms of the ion size effect, the mixed-alkali effect and lower concentration of Cs compared with Na in P0798 glass.

Self-Diffusion of 22Na and 137Cs in Simulated Nuclear Waste Glass. K.Nonaka, H.Nakajima, S.Mitsui, J.Echigoya: Materials Transactions, 2002, 43[4], 654-9

 

 

 Table 3

 Diffusion of 137Cs in P0798 (SiO2-14.2B2O3-5Al2O3-3Li2O-3CaO-3wt%ZnO) Glass

 

 

Phase

Temperature (K)

D (m2/s)

below Tg

758

1.73 x 10-21

below Tg

745

9.68 x 10-22

below Tg

733

4.21 x 10-22

below Tg

713

1.60 x 10-22

above Tg

818

6.39 x 10-19

above Tg

804

1.18 x 10-19

above Tg

802

1.02 x 10-19

above Tg

801

1.06 x 10-19

above Tg

795

4.69 x 10-20

above Tg

787

2.82 x 10-20

above Tg

774

8.38 x 10-21