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Thermodynamic study of (U-Pu-Zr-O-Fe) corium system

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HAL Id: cea-02489508

https://hal-cea.archives-ouvertes.fr/cea-02489508

Submitted on 24 Feb 2020

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Thermodynamic study of (U-Pu-Zr-O-Fe) corium system

A. Quaini, C. Gueneau, S. Gosse, T. Alpettaz, E. Brackx, A. Chocard, R. Domenger, D. Manara, K. Boboridis, P. Lajarge, et al.

To cite this version:

A. Quaini, C. Gueneau, S. Gosse, T. Alpettaz, E. Brackx, et al.. Thermodynamic study of (U-Pu-Zr-O-Fe) corium system. International Conference on Computer Coupling of Phase Diagrams and Thermochemistry - CALPHAD XLIV, May 2015, Loano, Italy. �cea-02489508�

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Thermodynamic sudy of the (U-Pu-Zr-O-Fe)

Calphad 2015, 31 May-5 June, Loano, Italy

Andrea Quaini

1

, Christine Guéneau

1

, Stéphane Gossé

1

, Thierry Alpettaz

1

, Emmanuelle Brackx

2

, Alexis Chocard

2

,

Renaud Domenger

2

, Dario Manara

3

, Kostantinos Boboridis

3

, Patrick Lajarge

3

, Fiqiri Hodaj

4

1 DEN,DPC,SCCME,LM2T, CEA Saclay, 91191Gif-sur-Yvette Cedex, France,

2 DEN,DTEC,SGCS,LMAC, CEA Marcoule, 30207 Bagnols sur Cèze Cedex, France

3ITU, JRC, EC, 76125 Karlsruhe, Germany

4 SIMAP, UMR CNRS 5266, 38402 Saint Martin d’Hères, France

CONTEXT AND PURPOSE OF THE WORK

In case of severe accident in a pressurized water reactor (PWR), the nuclear oxide fuel (UO2±x or (U,Pu)O2±x) could react with the Zr-alloy cladding and subsequently with the stainless steel vessel to form a mixture of solid and liquid phases, designated as “corium”. The high temperature thermodynamic properties of this complex mixture have to be properly established to predict the corium behaviour during a severe accident. The approach is to develop a thermodynamic database using Calphad method on the (U-Pu-Zr-O-Fe) system that is representative for UO2±x or (U,Pu)O2±x fuel, Zr-alloy cladding and steel vessel. A critical analysis of the available experimental data was first performed. Then an experimental work was carried out to provide new phase diagram data in U-Zr-O, Fe-Zr-O, UO2-PuO2-ZrO2 sub-systems. Heat treatments in the U-Zr-O and Fe-Zr-O systems allowed for highlighting the existence of miscibility gaps in the liquid state in both systems. The advanced laser heating setup developed in ITU was used to measure temperatures of solid/liquid transitions in the UO2-PuO2-ZrO2 sub-system. All the experimental data together with literature data were used to improve the thermodynamic modelling of the (U-Pu-Zr-O-Fe) system. Both experimental and calculated results will be presented on the different corium systems.

MISCIBILITY GAP IN THE U-ZR-O SYSTEM

- 4 samples (mixtures of U, Zr, ZrO2) heated at 2567 K for 45 minutes in W crucibles  2 metallic and oxide liquids

- Characterization using SEM, EDS, WDS  experimental tielines

Laser heating setup in ITU

(Karlsruhe)

SOLIDIFICATION TEMPERATURE IN UO

2

-ZrO

2

-PuO

2

SYSTEM

CONCLUSION

 New experimental results on corium

- Tielines in liquid miscibility gap of U-Zr-O, U-Zr-O-Fe systems

- Phase transition temperature measurements in U-Zr-O, Fe-Zr-O and UO2-PuO2-ZrO2 systems (ITU)

- Development of the ATTILHA new laser heating setup

 Improvement of the thermodynamic

modelling

- UO2-PuO2-ZrO2 system - U-Pu-Zr-Fe-O system

 Application calculations for severe accidents

- Solidification paths to interpret the quenched microstructure

- Corium/concrete interaction (using TAF-ID database for concrete systems)

ATTILHA SETUP DEVELOPMENT

- Phase transition temperature measurements in Al2O3-ZrO2 system (10 mol. % ZrO2)

Radiativeheat transfer

Metallic layer

Oxidicpool Q

Oxidiccrust Lower head

Maximum heat flux

Radiativeheat transfer

Metallic layer Oxidicpool Q Metallic layer Oxidicpool Q Oxidiccrust Lower head oxide zone metallic zone interface 200 µm

Böhler et al. J Alloy Comp 2014

Laser heating setup in ITU (Karlsruhe)

Sample compositions

Thermogram of sample 3 under 0,3 MPa Argon

a b c d e f g h i j k l 2600 2650 2700 2750 2800 2850 2900 Air M e lti n g tem p e ra tur e / K sequence of shots Ar + 6% H2 Ar

(UO2)45(PuO2)10(ZrO)45

Oxidation

Influence of the atmosphere

UO2 poor samples

Reduced under Argon  T liq 

UO2 rich samples

Oxidized under Air  T liq  2-ch pyrometer Laser CO2 Cu-mirror HgCdTe Detector (filtered @10µm) Levitation gas (Ar or Air) Filtered @ 3.99 μm Ch1: 0.8 μm Ch2: 1.05 μm sample During cooling  Solidification During heating  Melting

Microstructure of the quenched sample

Infrared image

of the levitating sample

Thermogram under Argon

For UO2 rich samples  Argon is recommended For UO2 poor samples  Air is recommended Liquid tetragonal monoclinic vessel (steel) fuel sheath (zircaloy) fuel pellet (UO2) Evolution of the sample overall composition due to « UO » vaporization

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