Titlebook: Equation of State of Uranium Dioxide; Data Collection Claudio Ronchi,Igor Lvovitch Iosilevski,Eugene Sol Book 2004 Springer-Verlag Berlin H

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Hilbrand Haak,Aryanti Radyowijatiorating uranium dioxide, and then extended, through a more complicated numerical procedure, to evaluate the non-congruent coexistence of vapour and liquid phases. The results of these calculations are described in the following sections.

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Ionic Models for Liquid Urania,that they are fully determined by the mere definition of their charges, and no other parameter is required to specify their thermodynamic quantities at any temperature. Furthermore, explicit relationships between some of them can be established, having an absolutely general validity for all these substances.

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Application of the Chemical Model within the van der Waals Approximation,orating uranium dioxide, and then extended, through a more complicated numerical procedure, to evaluate the non-congruent coexistence of vapour and liquid phases. The results of these calculations are described in the following sections.

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s the major problems in reactor safety guards by giving the In the beginning of the 1990’s, in the course of the events which were rapidly cha- ing the political con?guration of the East European countries, the crisis which - vested the vast research apparatus of the former Soviet Union was entailin

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Book 2004 crisis which - vested the vast research apparatus of the former Soviet Union was entailing con- quences whose dimension and depth were immediately realized by the international scienti?c community. In the same years, however, the most important branch of nuclear energy - searchanddevelopment,inpart

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Gas-Liquid Coexistence in Uranium Dioxide,hermodynamic potential is a linear combination of the thermodynamic potentials of the single phases. For example, if only two phases exist, ., liquid and vapour (for definiteness under isothermal — isochoric conditions), the thermodynamic potential (Helmholtz free energy) can be expressed as:

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Thermodynamic Properties of UO2, as Predicted by the New Equation of State,er 2; the details of its structure are explained and discussed in Chapters 3 to 6. After a recapitulation of the fundamental hypotheses and a summary of the main features, this Chapter is dedicated to the presentation of an extensive set of numerical calculations and to the comparison with predictions of alternative models.

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