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

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9.1 Neptunium halide compounds 1519.1.4 Neptunium bromide compounds9.1.4.1 NpBr 3 (cr)NpBr 3 (cr) exists in two crystal modifications, the hexagonal structure isomorphouswith UBr 3 (cr) (space group P6 3 /m) <strong>and</strong> the orthorhombic form (TbCl 3 -type, spacegroup Cmcm) in which PuBr 3 (cr) crystallises.9.1.4.1.a Enthalpy <strong>of</strong> formationHurtgen [78HUR] has measured the enthalpy <strong>of</strong> solution <strong>of</strong> the hexagonal form<strong>of</strong> NpBr 3 (cr) to be −(161.4 ± 2.0) kJ·mol −1 in oxygen-free 10 −3 M HCl<strong>and</strong> −(158.8 ± 0.9) kJ·mol −1 in oxygen-free 0.1 M HCl. The partial molarenthalpy <strong>of</strong> formation <strong>of</strong> HBr in HCl solutions is assumed to be the same asin HBr solutions <strong>of</strong> the same molality, which have been recalculated from theenthalpy <strong>of</strong> dilution data given by Parker [65PAR], <strong>and</strong> are −(121.33 ± 0.15)<strong>and</strong> −(120.71 ± 0.15) [2000RAN/FUG]. These <strong>and</strong> the currently assessed valuefor f Hm ◦ (Np3+ , aq, 298.15 K) = −(527.2 ± 2.1) kJ·mol −1 assumed to be thesame as in 10 −3 <strong>and</strong> 0.1 M HCl give the values <strong>of</strong> −(729.8 ± 2.9) kJ·mol −1 <strong>and</strong>−(730.5 ± 2.9) kJ·mol −1 for f Hm ◦ (NpBr 3, cr, hex, 298.15 K) from these solutions.The selected value is the weighted mean f H ◦ m (NpBr 3, cr, hex, 298.15 K) = −(730.2 ± 2.9) kJ·mol −1The use <strong>of</strong> the infinite dilution value for f H ◦ m (Np3+ , aq, 298.15 K) in 0.001<strong>and</strong> 0.1 M HCl solutions in these calculations has been justified by Fuger et al.[83FUG/PAR] on the grounds that the enthalpies <strong>of</strong> formation <strong>of</strong> all the actinidetrivalent ions vary by less than 0.5 kJ·mol −1 between 0.1 M HCl solutions <strong>and</strong> theinfinitely dilute solution. We accept this reasoning, but have increased the uncertaintyon the value derived from the measurement in 0.1 M HCl.9.1.4.1.bSt<strong>and</strong>ard entropy <strong>and</strong> heat capacityThere are no low-temperature measurements <strong>of</strong> the heat capacity <strong>of</strong> NpBr 3 (cr),<strong>and</strong> the st<strong>and</strong>ard entropy is derived from three reasonably consistent estimates by[2000RAN/FUG]. From these three estimates <strong>of</strong> 206.1, 194.9, 195.6 J·K −1·mol−1 ,the selected value is biased towards the lower estimates [2000RAN/FUG]Sm ◦ (NpBr −13, cr, hex, 298.15 K) = (196 ± 8) J·K−1·mol9.1.4.1.cHigh temperature heat capacityLacking experimental data, the heat capacity <strong>of</strong> NpBr 3 (cr) is assumed to be similar toUBr 3 (cr) <strong>and</strong> those estimated for PuBr 3 (cr) by this review. The values suggested forNpBr 3 (cr) are:Cp,m ◦ (NpBr 3, cr, hex, T) = (101.23 + 20.68 × 10 −3 T − 3.2 × 10 5 T −2 −1) J·K−1·mol

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