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Heat Capacity and Thermodynamic Properties of Plutonium Dioxide

Owen L. Kruger, H. W. Savage

Open publisher page 47 citations

Abstract

Changes in the heat content of PuO2 were measured from 192° to 1400°K with an isothermal drop calorimeter. The enthalpy curve, which was a smooth function of temperature, is described by the equation HT − H298 = − 8468 + 22.18T + 1.040 × 10−4T2 + 4.935 × 105T−1. The first derivative of this equation gave the heat-capacity relation, Cp = 22.18 + 2.080 × 10−4T−4.935 × 105T−2. At 298°K this equation agrees with previously reported low-temperature measurements made with an adiabatic calorimeter. These high- and low-temperature data were combined to obtain standard-state heat content, heat capacity, entropy, and Gibbs free energy functions to 1800°K. Measurements by other investigators show that PuO2 has a temperature-independent magnetic susceptibility below 1000°K. This behavior explains the comparatively low entropy of 16.34 cal mole−1·deg−1 for stoichiometric PuO2 at 298°K, which is somewhat greater than the value found for ThO2 and considerably less than the values for UO2 and NpO2.

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What this paper is about

Changes in the heat content of PuO2 were measured from 192° to 1400°K with an isothermal drop calorimeter. The enthalpy curve, which was a smooth function of temperature, is described by the equation HT − H298 = − 8468 + 22.18T + 1.040 × 10−4T2 + 4.935 × 105T−1. The first derivative of this equation gave the heat-capacity relation, Cp = 22.18 + 2.080 × 10−4T−4.935 × 105T−2. At 298°K this equation agrees with previously reported low-temperature measurements made with an adiabatic calorimeter. These high- and low-temperature data were combined to obtain standard-state heat content, heat capacity, entropy, and Gibbs free energy functions to 1800°K. Measurements by other investigators show that PuO2 has a temperature-independent magnetic susceptibility below 1000°K. This behavior explains the comparatively low entropy of 16.34 cal mole−1·deg−1 for stoichiometric PuO2 at 298°K, which is somewhat greater than the value found for ThO2 and considerably less than the values for UO2 and NpO2.

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Available abstract

Changes in the heat content of PuO2 were measured from 192° to 1400°K with an isothermal drop calorimeter. The enthalpy curve, which was a smooth function of temperature, is described by the equation HT − H298 = − 8468 + 22.18T + 1.040 × 10−4T2 + 4.935 × 105T−1. The first derivative of this equation gave the heat-capacity relation, Cp = 22.18 + 2.080 × 10−4T−4.935 × 105T−2. At 298°K this equation agrees with previously reported low-temperature measurements made with an adiabatic calorimeter. These high- and low-temperature data were combined to obtain standard-state heat content, heat capacity, entropy, and Gibbs free energy functions to 1800°K. Measurements by other investigators show that PuO2 has a temperature-independent magnetic susceptibility below 1000°K. This behavior explains the comparatively low entropy of 16.34 cal mole−1·deg−1 for stoichiometric PuO2 at 298°K, which is somewhat greater than the value found for ThO2 and considerably less than the values for UO2 and NpO2.

Key concepts: Heat capacity, Thermodynamics, Adiabatic process, Gibbs free energy, Calorimeter (particle physics), Isothermal process, Enthalpy, Calorimetry

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