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

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304 16. Plutonium aqua ions298.15 K) = −(290.91 ± 0.85) kJ·mol −1 is used to calculate f G ◦ m from the valuesselected for Pu 3+ <strong>and</strong> CODATA auxiliary values. f G ◦ m (PuO2+ 2, aq, 298.15 K) = −(762.4 ± 2.8) kJ·mol−1Using the Gibbs-Helmholtz relation <strong>and</strong> r Hm ◦ = −(822.0 ± 6.6) kJ·mol−1 , r Sm ◦ (16.4, 298.15 K) = −(200.2 ± 22.1) J·K−1·mol−1 . From this number, thest<strong>and</strong>ard molar entropy value <strong>of</strong> PuO 2+2is calculated as:S ◦ m (PuO2+ 2 , aq, 298.15 K) = −(71.2 ± 22.1) J·K−1·mol −1 .using Sm ◦ (Pu,α,298.15 K) = (54.46 ± 0.80) J·K−1·mol−1 from this review <strong>and</strong>CODATA auxiliary values.Lemire <strong>and</strong> Campbell [96LEM/CAM] have used the results <strong>of</strong> their study <strong>of</strong> apparentmolar heat capacities <strong>of</strong> NpO 2 ClO 4 (aq) with values <strong>of</strong> the partial molar heat capacities<strong>of</strong> other electrolytes [89HOV/NGU, 96LEM/CAM2] to estimate the variation <strong>of</strong>the potential <strong>of</strong> the Pu(VI)/Pu(V) couple as a function <strong>of</strong> temperature. The apparentmolar heat capacities <strong>of</strong> PuO 2+2<strong>and</strong> PuO + 2as a function <strong>of</strong> temperature were assumedequal to those for UO 2+2<strong>and</strong> NpO + 2, respectively [89HOV/NGU, 96LEM/CAM].The mean value proposed by Capdevila <strong>and</strong> Vitorge [95CAP/VIT] for r C p,m (16.8) is approximately −400 J·K −1·mol−1 . This was calculated by doubledifferentiation <strong>of</strong> a smoothed function <strong>of</strong> EVI/V ◦ (T) (based on experimental potentialmeasurements for temperature from 5 to 65 ◦ C), <strong>and</strong> is much more negative than the−70 J·K −1·mol−1 calculated by the method <strong>of</strong> Lemire <strong>and</strong> Campbell [96LEM/CAM].The uncertainties in that method cannot accommodate the Capdevila <strong>and</strong> Vitorge value[95CAP/VIT], <strong>and</strong> suggest the uncertainty in the entropy value proposed for that workshould also be increased. To a first approximation, this review accepts that the partialmolar heat capacities <strong>of</strong> all the aqueous dioxoactinide(V) <strong>and</strong> dioxoactinides(VI)ions can be assumed identical to those determined for UO 2+2<strong>and</strong> NpO + 2 , respectively[89HOV/NGU, 96LEM/CAM].16.3 PuO + 2The st<strong>and</strong>ard Gibbs energy <strong>of</strong> formation <strong>of</strong> the dioxo<strong>plutonium</strong>(V) cation is calculatedby this review from the st<strong>and</strong>ard potential <strong>of</strong> the reactionPuO 2+2+ e − Å PuO + 2(16.7)Several independent determinations <strong>of</strong> the PuO 2+2 /PuO+ 2potential in perchloricacid solution are available. They are summarised in Table 16.2. The formal potentialsin 1 M HClO 4 at 25 ◦ C were determined by Rabideau [56RAB],<strong>and</strong>byCapdevilaet al. [92CAP, 92CAP/VIT, 95CAP/VIT], as E ◦′ = (0.9164 ± 0.0002) V, <strong>and</strong>(0.912 ± 0.007) V, respectively.The value <strong>of</strong> Riglet, Robouch <strong>and</strong> Vitorge [89RIG/ROB], (0.941 ± 0.0052) V,was determined at 20 ◦ C, <strong>and</strong> not at 25 ◦ C, the st<strong>and</strong>ard temperature. They derived

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