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

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98 7. Neptunium aqua ionsnon-systematic values for Sm ◦ (MO+ 2(aq), M = U, Np, Pu, Am) (respectively, -25, -46,2<strong>and</strong>-21J·K −1·mol−1 , cf. Section 16.3 <strong>and</strong> References [92GRE/FUG, 95SIL/BID])were not indicated in previous reviews [76FUG/OET, 86MOR] that relied moreheavily on estimates. The differences in the entropy values for these key ions appearto be beyond those easily attributable to specific experimental uncertainties, <strong>and</strong> needto be confirmed or refuted by further experimental work.Using f Hm ◦ (Np4+ , 298.15 K) = −(556.0 ± 4.2) kJ·mol −1 , f G ◦ m (Np4+ ,298.15 K) =−(491.8 ± 5.6) kJ·mol −1 (cf. Section 7.4) <strong>and</strong> CODATA auxiliary data,the following selected values are calculated: f Hm ◦ (NpO+ 2, aq, 298.15 K) = −(978.2 ± 4.6) kJ·mol−1 f G ◦ m (NpO+ 2, aq, 298.15 K) = −(907.8 ± 5.6) kJ·mol−1Values <strong>of</strong> ionic apparent molar heat capacities vary strongly with temperature, <strong>and</strong> to asomewhat lesser degree with ionic strength. The influence <strong>of</strong> heat capacity on the Gibbsenergy <strong>of</strong> reaction is usually too small to determine r C p,m or r C p,m (T) from second<strong>and</strong> higher order derivatives <strong>of</strong> functions describing the temperature dependence <strong>of</strong>solubilities or potentials. Lemire <strong>and</strong> Campbell [93LEM/CAM, 96LEM/CAM] havereported apparent molar heat capacities <strong>of</strong> NpO 2 ClO 4 (aq) as a function <strong>of</strong> temperature(18 to 100 ◦ C) for a limited range <strong>of</strong> ionic strengths (0.05 to 0.22 m). The extrapolatedvalues for the partial molar heat capacities can be expressed as:C ◦ p,m,2 (NpO 2ClO 4 , aq, T) = (3.56770 × 10 3 − 4.95931T−6.32344 × 10 5 T −1 ) J·K−1·mol−1The value <strong>of</strong> C ◦ p,m,2 (NpO 2ClO 4 , aq) at 298.15 K is −(32 ± 25) J·K −1·mol−1 ,where the uncertainty is assigned in the present review, <strong>and</strong> comparable uncertaintiesapply to values throughout the temperature range <strong>of</strong> the measurements. This value<strong>and</strong> the equation above are accepted in the present review. For the usual st<strong>and</strong>ard state(C ◦ p,m,2 (H+ , aq, 298.15 K) = 0J·K −1·mol−1 ),usingC ◦ p,m,2 (HClO 4, aq, 298.15 K) =−27.8 J·K −1·mol−1 [96LEM/CAM2] the value <strong>of</strong> the partial molar heat capacity,C ◦ p,m,2 (NpO+ 2 , aq, 298.15 K) =−(4 ± 25) J·K−1·mol−1 , is calculated.Lemire <strong>and</strong> Campbell [96LEM/CAM] have used their values for C ◦ p,m,2 (NpO 2ClO 4 ,aq, T) 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> theNp(VI)/Np(V) couple as a function <strong>of</strong> temperature. The apparent molar heatcapacity as a function <strong>of</strong> temperature <strong>of</strong> NpO 2+2was assumed equal to that <strong>of</strong>UO 2+2[89HOV/NGU, 96LEM/CAM]. The uncertainties in values <strong>of</strong> r C p,m (7.4, T)estimated in that way are estimated here as ±70 J·K −1·mol−1 .7.4 Np 4+The thermodynamic quantities for Np 4+ are derived from the value <strong>of</strong> the entropy basedon the solubility <strong>and</strong> the enthalpy <strong>of</strong> dissolution <strong>of</strong> NpO 2 (NO 3 ) 2·6H 2 O(s) in water, the

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