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chemical thermodynamics of neptunium and plutonium - U.S. ...

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334 17. Plutonium oxygen <strong>and</strong> hydrogen compounds <strong>and</strong> complexesThese are based on measurements by Riley [70RIL] in 1 atm oxygen, Lyon <strong>and</strong>Bailey [67LYO/BAI], Chikalla et al. [64CHI/MCN], <strong>and</strong> comparison with urania. Wehave also taken for the value <strong>of</strong> the heat capacity <strong>of</strong> liquid PuO 2Cp,m ◦ (PuO −12, l) = 131 J·K−1·molas suggested by Glushko et al. [82GLU/GUR]. It should be emphasised again thatPuO 2 will only melt congruently at very high pressures <strong>of</strong> oxygen.17.2.1.2.cEnthalpy <strong>and</strong> Gibbs energy <strong>of</strong> formationThere is very good agreement between the several values for the enthalpy <strong>of</strong> combustion<strong>of</strong> <strong>plutonium</strong> in oxygen by Popov <strong>and</strong> Ivanov [57POP/IVA] (−(1056.0 ±4.0) kJ·mol −1 ), Holley et al. [58HOL/MUL] (−(1058.0 ± 1.6) kJ·mol −1 ) <strong>and</strong> Johnsonet al.[69JOH/DEV](−(1055.70 ± 0.71) kJ·mol −1 ). We select the value: f H ◦ m (PuO 2, cr, 298.15 K) = −(1055.8 ± 1.0) kJ·mol −1givenbyGlushkoet al. [82GLU/GUR], which is biased towards the appreciably moreprecise value by Johnson et al.[69JOH/DEV]. The derived Gibbs energy <strong>of</strong> formation<strong>of</strong> PuO 2 (cr) is thus f G ◦ m (PuO 2, cr, 298.15 K) =−(998.113 ± 1.031) kJ·mol −117.2.1.2.dSolubility measurementsThe ratios <strong>of</strong> the solubility products <strong>of</strong> PuO 2 (cr) <strong>and</strong> hydrated PuO 2 (cr) found in thestudies <strong>of</strong> Kim <strong>and</strong> Kanellakopulos [89KIM/KAN2]<strong>and</strong>Raiet al.[80RAI/SER] appearto be similar. The value from Rai et al.[80RAI/SER] is subject to the same problems asthe value for hydrated PuO 2 from the same study [84RAI] (cf. Section 17.2.2.3). Thesolubility product reported by Kim <strong>and</strong> Kanellakopulos [89KIM/KAN2] forPuO 2 (cr)appears to be a good measurement for a batch experiment on a radioactive solid. However,it is not surprising that the value <strong>of</strong> K s,0 is greater than the thermodynamic constantbased on bulk (rather than surface) properties <strong>of</strong> the crystalline material (see Section17.2.2.3).17.2.1.3 Pu 2 O 3 (cr)17.2.1.3.aCrystal structurePu 2 O 3 (cr) has the hexagonal type-A rare earth sesquioxide structure (space groupP3m1) with a = 3.841 × 10 −10 m, c = 5.958 × 10 −10 m <strong>and</strong> a calculated density<strong>of</strong> 11.47 g·cm −3 . As discussed in [67IAE], there is some evidence for the occurrence<strong>of</strong> a disordered variant <strong>of</strong> this structure in some samples <strong>of</strong> Pu 2 O 3 (cr), but it is notknown whether this is due to the presence <strong>of</strong> impurities or a change in composition.

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