Thermodynamic modelling of the C-U and B-U binary systems

被引:60
作者
Chevalier, PY [1 ]
Fischer, E [1 ]
机构
[1] INPG, CNRS, UMS THERMA, F-38402 St Martin Dheres, France
关键词
Corium;
D O I
10.1016/S0022-3115(00)00713-3
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The thermodynamic modelling of the carbon-uranium (C-U) and boron-uranium (B-U) binary systems is being performed in the framework of the development of a thermodynamic database for nuclear materials, for increasing the basic knowledge of key phenomena which may occur in the event of a severe accident in a nuclear power plant. Applications are foreseen in the nuclear safety held to the physico-chemical interaction modelling, on the one hand the invessel core degradation producing the cerium (fuel, zircaloy, steel, control rods) and on the other hand the ex-vessel molten cerium-concrete interaction (MCCI). The key O-U-Zr ternary system, previously modelled, allows us to describe the first interaction of the fuel with zircaloy cladding. Then, the three binary systems Fe-U, Cr-U and Ni-U were modelled as a preliminary work for modelling the O-U-Zr-Fe-Cr-Ni multicomponent system, allowing us to introduce the steel components in the cerium. In the existing database (TDBCR, thermodynamic data base for cerium), Ag and In were introduced for modelling AIC (silver-indium-cadmium) control rods which are used in French pressurized water reactors (PWR). Elsewhere, B4C is also used for control rods. That is why it was agreed to extend in the next years the database with two new components, B and C. Such a work needs the thermodynamic modelling of all the binary and pseudo-binary sub-systems resulting from the combination of B, B2O3 and C with the major components of TD B CR, O-U-Zr-Fe-Cr-Ni-Ag-In-Ba-La-Ru-Sr-Al-Ca-Mg-Si + Ar-H. The critical assessment of the very numerous experimental information available for the C-U and B-U binary systems was performed by using a classical optimization procedure and the Scientific Group Thermodata Europe (SGTE). New optimized Gibbs energy parameters are given, and comparisons between calculated and experimental equilibrium phase diagrams or thermodynamic properties are presented. The self-consistency obtained is quite satisfactory. (C) 2001 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:100 / 129
页数:30
相关论文
共 99 条
[1]   SPECIFIC HEAT OF UC AND UN [J].
AFFORTIT, C .
JOURNAL OF NUCLEAR MATERIALS, 1970, 34 (01) :105-&
[2]  
AKHACHINSKI VV, 1970, ATOM ENERG, V29, P439
[3]  
ALCOCK CB, 1962, THERMODYNAMICS NUCL, P563
[4]  
ALTOCK C, 1962, THERMODYNAMICS NUCL, P563
[5]  
[Anonymous], 1969, HIGH TEMP SCI
[6]  
Anselin F., 1964, CARBIDES NUCLEAR ENE, VI, P113
[7]   STRUCTURES OF CALCIUM DICARBIDE AND URANIUM DICARBIDE BY NEUTRON DIFFRACTION [J].
ATOJI, M ;
MEDRUD, RC .
JOURNAL OF CHEMICAL PHYSICS, 1959, 31 (02) :332-337
[8]   CARBON POSITIONS IN URANIUM CARBIDES [J].
AUSTIN, AE .
ACTA CRYSTALLOGRAPHICA, 1959, 12 (02) :159-161
[9]   STANDARD MOLAR FREE ENERGY OF FORMATION OF URANIUM DICARBIDE AND URANIUM SESQUICARBIDE BY ELECTROMOTIVE FORCE MEASUREMENTS [J].
BEHL, WK ;
EGAN, JJ .
JOURNAL OF THE ELECTROCHEMICAL SOCIETY, 1966, 113 (04) :376-&
[10]  
BENESOVSKY F, 1961, PLANSEEBER PULVERMET, V9, P65