Published 1980 | Version v1
Book

The thermodynamic functions of gaseous actinide elements. Effects of unobserved energy levels

Creators

  • 1. UKAEA Atomic Energy Research Establishment, Harwell. Materials Development Div.

Description

The actinide gases have a large number of unobserved energy states - up to 3 x 106 for Pu(g) - which could contribute to the partition function and its derivatives, from which the thermal functions of these gases are calculated. Existing compilations have simply ignored these levels. By making reasonable assumptions as to the distribution of these energy states, their effect on the functions can be calculated. It is concluded that the existing compilations will be inadequate above approximately 2000 K. The effect is particularly marked on the heat capacity. For example, when unobserved levels for Pu(g) are included, the heat capacity of Pu(g) reaches a maximum value of more than 12R at 3200 K. Similar considerations will apply to the gaseous actinide ions. (author)

Additional details

Publishing Information

Publisher
IAEA.
Imprint Place
Vienna
ISBN
92-0-040080-9
Imprint Title
Thermodynamics of nuclear materials 1979
Imprint Pagination
v. 1 586 p.
Series
Proceedings series.
Journal Page Range
v. 1 p. 197-215.

Conference

Title
International symposium on thermodynamics of nuclear materials.
Dates
29 Jan - 2 Feb 1979.
Place
Juelich, Germany, F.R.

INIS

Country of Publication
International Atomic Energy Agency (IAEA)
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
12640698
Subject category
S37: INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY;
Resource subtype / Literary indicator
Conference
Descriptors DEI
ELECTRONIC SPECIFIC HEAT; ENERGY LEVELS; FREE ENTHALPY; PARTITION FUNCTIONS; PLUTONIUM; TEMPERATURE DEPENDENCE; ULTRAHIGH TEMPERATURE; URANIUM; VERY HIGH TEMPERATURE
Descriptors DEC
ACTINIDES; ELEMENTS; ENERGY; FUNCTIONS; METALS; PHYSICAL PROPERTIES; SPECIFIC HEAT; THERMODYNAMIC PROPERTIES; TRANSURANIUM ELEMENTS

Optional Information

Secondary number(s)
IAEA-SM--236/39.