A method derived by Kelly71 is often used in the prediction ofirradiated graphite thermal conductivity
in the assessment of UK reactor cores. The thermal resistivity, 1/K(T), induced because of irradiation as a function of temperature, T can be given by the difference between the thermal resistivity due to fast neutron damage, and the unirradiated thermal resistivity:
1 _ 1 1
K(T)_ Kjt) ~ K0(T)
However,
and as Ka ^ Ka Ka is assumed to dominate in polycrystalline graphite, Kai(T) = Ki(T) and Kai(30) = K*(30) = Kirr(30), and hence,
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The addition in these two factors in this way appears to be arbitrary as the author does not know of any validation of this method. Other methods do exist, but they depend on many more measurements
of thermal conductivity at various irradiation and
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measurement temperatures.
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The irradiation-induced fractional changes in thermal resistivity measured at 30 °C are available for graphite irradiated at various temperatures, Tirr. Therefore, for graphite irradiated and measured at 30 °C, we can write
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