Abstract:A comprehensive review of the thermodynamic properties of the oxide compounds of the lanthanide and actinide elements is presented. The available literature data for the solid, liquid, and gaseous state have been analysed and recommended values are presented. In case experimental data are missing, estimates have been made based on the trends in the two series, which are extensively discussed.
“…Actinide dioxide melting enthalpy values assessed by Konings et al [29] are used to calculate the optimised solidus and liquidus plotted in figure 7 together with the current experimental data. It is evident that the current experimental data relative to plutonia-rich compositions deviate from such phase diagram.…”
a b s t r a c tA laser heating approach combined with fast pyrometry in a thermal arrest method was used to provide new data for the melting/solidification phase transition in mixed (PuO 2 + ThO 2 ) at high temperature. At low concentration of ThO 2 in PuO 2 a minimum in the solidification temperature in the pseudo binary (PuO 2 + ThO 2 ) was observed. The minimum was found around a composition with 5 mol% ThO 2 . Phase transition temperatures of other compositions are closer to an ideal solution behaviour. To detect changes in the material a complete investigation with electron microscopy, Raman spectroscopy and powder X-ray diffraction was done. Raman vibration modes were found, that are characteristic for materials containing PuO 2 , and high temperature segregation effects during solidification were described. The results obtained in the present work are compared to other mixed actinide dioxides and compared to the ideal solution case for this system. The presented results show the importance of the hightemperature oxygen chemistry in this actinide oxide phase.
“…Actinide dioxide melting enthalpy values assessed by Konings et al [29] are used to calculate the optimised solidus and liquidus plotted in figure 7 together with the current experimental data. It is evident that the current experimental data relative to plutonia-rich compositions deviate from such phase diagram.…”
a b s t r a c tA laser heating approach combined with fast pyrometry in a thermal arrest method was used to provide new data for the melting/solidification phase transition in mixed (PuO 2 + ThO 2 ) at high temperature. At low concentration of ThO 2 in PuO 2 a minimum in the solidification temperature in the pseudo binary (PuO 2 + ThO 2 ) was observed. The minimum was found around a composition with 5 mol% ThO 2 . Phase transition temperatures of other compositions are closer to an ideal solution behaviour. To detect changes in the material a complete investigation with electron microscopy, Raman spectroscopy and powder X-ray diffraction was done. Raman vibration modes were found, that are characteristic for materials containing PuO 2 , and high temperature segregation effects during solidification were described. The results obtained in the present work are compared to other mixed actinide dioxides and compared to the ideal solution case for this system. The presented results show the importance of the hightemperature oxygen chemistry in this actinide oxide phase.
“…The dioxides of the first three elements have the eight-coordinate fluorite structure. 42 At room temperature, hafnium dioxide has a monoclinic structure in which the hafnium atom is seven-coordinate. However, the cubic fluorite form is stable above 2870 K and there is an experimental value of 5.08 A for its unit cell parameter 51 (internuclear distance 2.20Å).…”
Section: Lattice Enthalpies Of Tetravalent Lanthanide Oxidesmentioning
confidence: 99%
“…Reviews of the enthalpies of formation of lanthanide trichlorides, 40,41 sesquioxides, 42 and aqueous ions 43 give the values shown in …”
Section: Lattice Enthalpies and Hydration Enthalpies Of Trivalent Commentioning
confidence: 99%
“…42 The values of 1/2L Ɵ (Ln 2 O 3 ) can be calculated from columns 4 and 7 of Since this estimate is a constant for each lattice enthalpy, it does not affect the variation, or the subshell break of 38 kJ mol 21 revealed by Fig. 9(C).…”
By interpolating a 4fq6s → 4fq7s transition within the sequence f1 → f14 rather than between f0 and f14, revised third and fourth ionization energies of the lanthanides have been obtained. The revised values, together with the second ionization energies calculated in a previous paper, are used to calculate values of the standard enthalpies of formation of the gaseous tripositive ions, ΔfHƟ(M3+,g), and of the lattice and hydration enthalpies of some lanthanide compounds and ions in the trivalent and tetravalent states. The displacements of f0 values from nearly smooth f1 → f14 variations exceed 30 kJ mol−1 and indicate substantial subshell breaks.
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