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

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A. Discussion <strong>of</strong> selected references 779the interaction coefficients are very similar for An = U, Np <strong>and</strong> Pu: ε(IV/III) =ε (An 4+ ,ClO − 4 ) − ε (An 3+ ,ClO − 4 ) = (0.35 ± 0.06) kg·mol−1 ,(0.35 ± 0.03) kg·mol −1 <strong>and</strong>(0.33 ± 0.05) kg·mol −1 respectively, <strong>and</strong> ε(VI/V) = ε (AnO2+2 ,ClO− 4 ) − ε (AnO + 2 ,ClO− 4 ) =(0.20 ± 0.06), (0.21 ± 0.03) <strong>and</strong> (0.22 ± 0.03) kg·mol −1 respectively. For <strong>plutonium</strong>the uncertainty in ε(IV/III) was reported as ±0.05 kg·mol −1 in Table 4, but as ±0.03kg·mol −1 in the abstract <strong>and</strong> in Table 2. The authors increased their uncertainties forsystematic errors (considering variation <strong>of</strong> the junction potential with temperature,ionic strength <strong>and</strong> temperature corrections to the st<strong>and</strong>ard potential <strong>of</strong> the referenceelectrode, <strong>and</strong> use <strong>of</strong> the SIT approximation). Re-evaluation carried out in conjunctionwith the present review led to ε(IV/III) = 0.22 kg·mol −1 with an uncertainty <strong>of</strong> ≤0.03, regardless <strong>of</strong> whether only the 25 ◦ C or the data for all temperatures, smoothed to25 ◦ C, were used. Previous ε values for the <strong>plutonium</strong> couples [89RIG/ROB] wererejected because interference between the two redox couples during the measurement<strong>of</strong> E ◦′ was suspected. Published E ◦′ <strong>and</strong> E ◦ data were discussed, <strong>and</strong> possibleexplanations <strong>of</strong> outliers were given. The E ◦′ <strong>and</strong> E ◦ values [95CAP/VIT] are in accordwith the ones selected in this review. This review selects <strong>and</strong> uses the ε valuesreported in this paper in preference to the SIT coefficients for Np <strong>and</strong> Pu species thathad been derived from [89RIG/ROB] <strong>and</strong> used previously [92GRE/FUG, 95SIL/BID].The influence <strong>of</strong> changes in temperature on interaction coefficients <strong>of</strong> reaction, ε,<strong>and</strong> the ionic strength correction applicable to the enthalpies <strong>and</strong> entropies <strong>of</strong> reactionsare also calculated in this work from the temperature <strong>and</strong> ionic strength dependence <strong>of</strong>the formal potentials <strong>of</strong> the <strong>plutonium</strong> reversible redox couples in acidic media.[95FAN/NEC]In this report a set <strong>of</strong> Pitzer coefficients is derived for Np(V) hydrolysis species <strong>and</strong>carbonate complexes for perchlorate <strong>and</strong> chloride media (based on data reported inearlier publications). See the discussions <strong>of</strong> [91KIM/KLE, 94MEI, 94NEC/KIM,94NEC/RUN] in this appendix.[95MOR/PRA]Pratopo’s data (also in [93PRA/MOR]) were obtained from experiments in which equilibriumwas probably not attained. Although equilibrium constants based on these datawere proposed in Pratopo’s thesis [93PRA], equilibrium constants for soluble speciesbased on these data are not accepted in the present review. All the published Np(VI)solubility measurements for these conditions ([CO 2−3] > 10 µM) are quite scattered.Some values plotted in log 10 -log 10 representation are parallel to those for UO 2 CO 3 (s)solubility curves over small domains; but extracting numbers from this type <strong>of</strong> observationleads to contradictions with other published solubility work. The slow transformation<strong>of</strong> one solid phase (NpO 2 CO 3 (s)) to another (Na 4 NpO 2 (CO 3 ) 3 (s)) could explainthese scattered results for a single series <strong>of</strong> measurements, since soluble species generallyattain equilibrium faster than transformation can occur within the bulk <strong>of</strong> the solidphase. Also see the comments in this appendix, for [93PRA/MOR, 98VIT/CAP].

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