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

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378 18. Plutonium group 17 (halogen) compounds <strong>and</strong> complexesSawant et al. [85SAW/CHA] also reported formation constants for the 1:3 complex,NpO 2 F − 3. Again, these constants reported for I = 0.1 M<strong>and</strong>I = 1 M are notcompatible with the specific ion interaction coefficients in Appendix B. For the correspondingU(VI) system we have ε(18.11, q = 3) =−0.52 kg·mol −1 [92GRE/FUG],<strong>and</strong> by using this value to correct the data <strong>of</strong> [85SAW/CHA] toI = 0 we obtainlog 10 β3 ◦ (18.11, q = 3) = 9.6 <strong>and</strong> 8.4 for the experiments carried out at I = 0.1 M<strong>and</strong> I = 1 M, respectively. In order to obtain consistent log 10 β3 ◦ values from thetwo determinations, we would have to use ε =+0.8 kg·mol −1 , <strong>and</strong> this would beincompatible with the commonly observed ionic strength dependence <strong>of</strong> comparableequilibria. The formation <strong>of</strong> NpO 2 F − 3needs closer examination, <strong>and</strong> no selection ismade at this time.The Gibbs energy <strong>of</strong> formation values are derived from the above selected constantsusing the selected f G ◦ m values for PuO2+2<strong>and</strong> F − . f G ◦ m (PuO 2F + , aq, 298.15 K) = −(1069.9 ± 3.1) kJ·mol −1 f G ◦ m (PuO 2F 2 , aq, 298.15 K) = −(1366.8 ± 4.1) kJ·mol −118.2.2 Aqueous <strong>plutonium</strong> chlorine complexes18.2.2.1 Aqueous <strong>plutonium</strong> chlorides18.2.2.1.a Aqueous Pu(III) chloridesQuantitative information on chloride complexation <strong>of</strong> Pu 3+ according to the equilibriaPu 3+ + qCl − Å PuClq 3−q(18.12)has been published by Ward <strong>and</strong> Welch [56WAR/WEL], Martin <strong>and</strong> White[58MAR/WHI] <strong>and</strong> Shiloh <strong>and</strong> Marcus [64SHI/MAR], <strong>and</strong> is summarised inTable 18.3. The study <strong>of</strong> Ward <strong>and</strong> Welch [56WAR/WEL] was carried out at ionicstrengths <strong>of</strong> 0.207, 0.5 <strong>and</strong> 1.0 M, respectively (cf. Appendix A). The formationconstant reported by Martin <strong>and</strong> White [58MAR/WHI] is not the result <strong>of</strong> anindependent measurement, but rather the result <strong>of</strong> an extrapolation <strong>of</strong> Ward <strong>and</strong>Welch’s [56WAR/WEL] value at I = 0.207 M (HCl) using the Davies equation.This value was used to derive the enthalpy <strong>of</strong> Reaction (18.12, q = 1) (see AppendixA <strong>and</strong> discussion below). The data <strong>of</strong> Ward <strong>and</strong> Welch [56WAR/WEL] reportedat “room temperature”, which Martin <strong>and</strong> White [58MAR/WHI] reported as 21 ◦ C, arethus corrected to t = 25 ◦ C(cf. Appendix A), using the enthalpy <strong>of</strong> reaction selectedbelow. Shiloh <strong>and</strong> Marcus [64SHI/MAR] used very high <strong>and</strong> variable ionic strengthsin their spectrophotometry experiments. These values cannot be used to select a formationconstant at I = 0. Giffaut [94GIF] noted that spectrophotometry is not a suitablemethod to study chloride complexation <strong>of</strong> Pu 3+ , due to the very small changes in theabsorption spectrum up to a chloride concentration <strong>of</strong> 4 M. It is probable that thiscomplexation could equally well be described as activity effects. The number <strong>of</strong> availableformation constants is insufficient for a linear extrapolation to I = 0. We adopt

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