Home / Publications / Journals / Nuclear Technology / Volume 68 / Number 3
Nuclear Technology / Volume 68 / Number 3 / March 1985 / Pages 336-343
Technical Paper / Nuclear Fuel / dx.doi.org/10.13182/NT85-A33579
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The transport or diffusion of uranium (as a stand-in for plutonium) was investigated under conditions approximating those of the primary coolant loop in a high-temperature gas-cooled reactor. Profiles were obtained for uranium penetration in H-451 graphite at temperatures ranging from 900 to 1400°C. Profile data for given temperatures were considered in terms of the following expression: where C is the concentration of uranium at time t, for distance x, into the pellet; C0 is a constant representing the uranium concentration at x = 0 for all t, and D is the diffusion coefficient. Diffusion coefficients for uranium initially present as dicarbide at 1000 and 1400°C were found to be defined by
For uranium initially present as dioxide at 900, 1000, and 1400°C, diffusion coefficients are defined by
where R is the gas constant and T is the temperature in degrees Kelvin.