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Security and Privacy Notice |
The recommended equations for the density of solid uranium dioxide are based on the lattice parameter value of 0.54704 nm obtained by Gronvold [1] at 293 K and the 1988 assessment of thermal expansion by D. G. Martin [2]. They are in agreement with the 1989 recommendations of Harding, Martin, and Potter [3]. The lattice parameter of Gronvold is in good agreement with recent measurements by Hutchings [4]. Assuming the molecular weight of UO2 is 270.0277, this lattic parameter gives a UO2 density at 293 K of 10.956 Mg/m-3. Applying the thermal expansion recommendation of Martin, the density at 273 K is 10.963 Mg/m-3.
The density as a function of temperature may be calculated from:

where rho(273) is the density at 273 K; L(273) and L(T) are the lengths at 273 K and at temperature T(K), respectively. The ratio of the length at 273 K to the length at temperature T(K) may be calculated from Martin's equations for the thermal expansion of solid UO2:

ERROR: The last factor in the previous equation should be 4.391E-13. Thanks to Jamie Higgs of the Dept. of Chemistry and Chemical Engineering at the Royal Military College of Canada for pointing this out.

The densities as a function of temperature of solid UO2 are given in Table 1.
From assessment of the available data on hyperstoichiometric uranium dioxide (UO2+x), Martin recommends using the same equations for the linear thermal expansion of UO2 and of UO2+x for x in the ranges 0 to 0.13 and 0.23 to 0.25. Therefore, equations (1) through (3) are recommended for the density of UO2+x for x in the ranges 0 to 0.13 and 0.23 to 0.25.
No data on the effect of burn-up on density or thermal expansion of UO2 are currently available. In the absence of data, equations (1) through (3) are recommended for UO2 during irradiation, in accord with the recommendation of Harding, Martin, and Potter [3].
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| Figure 1 |