experimental study of joint-oxyde-gaine (jog) systems in ... · the jog is a very-complex...

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Experimental study of Joint-Oxyde-Gaine (JOG) systems in Fast Neutron Reactors The JOG is a very-complex multicomponent system, including Cs 2 MoO 4 (major phase), Cs 2 Te, CsI, Cs 2 I 2 , but the exact composition is still not well-known. This work aims to obtain reliable experimental data for this multi-element system and use them to develop thermodynamic models based on the CALPHAD methodology. Context of the study The present study was performed in the framework of the European INSPYRE project, dedicated to the investigation of the (U,Pu)O 2 fuel behaviour under irradiation in Generation-IV Sodium-cooled Fast Reactors (SFRs) and Lead-cooled Fast Reactors (LFRs) [1]. Due to the very high thermal gradients in SFRs and LFRs (~ 450 K·mm -1 ), the volatile fission products generated during irradiation (e.g. Cs, I, Te, Mo) migrate from the center of the fuel pin (~2300 K) towards the pellet edge (~973 K), and accumulate in the space between fuel and cladding, forming an oxide layer of a few hundred micrometers, the so-called JOG layer (Joint Oxide Gaine) [2]. Lattice parameters evolution with composition and temperature were investigated using X-ray diffraction. The thermal expansion of Cs 2 TeO 4 (α V ~107.9·10 -6 K -1 ) is much higher than that of UO 2 (α V ~32.4·10 -6 K -1 ) [4]. Enthalpies of melting of key compounds were measured using differential scanning calorimetry (DSC) . These differed in some cases quite substantially from computed values in the available CALPHAD model [3]. Study of the Cs-Mo-O system Enthalpies of formation of Cs 2 Mo 2 O 7 and Cs 2 Mo 3 O 10 were determined using solution calorimetry. Cs 2 Mo 2 O 7 + n 1 CsOH = sol. 1 2MoO 3 + n 2 CsOH = sol. 1 Mo + 3/2O 2 = MoO 3 2Cs + 2H 2 O = 2CsOH + H 2 H 2 + 1/2O 2 = H 2 O 2Cs + 2Mo + 7/2O 2 = Cs 2 Mo 2 O 7 = . ± . / Study of Cs 2 (Te,Mo)O 4 solid solutions Structural investigations were performed using neutron diffraction at the PEARL beamline. Cs 2 TeO 4 is isostructural with Cs 2 MoO 4 , i.e. orthorhombic in space group Pnma. Phase diagram data in the Cs 2 TeO 4 -Cs 2 MoO 4 section and enthalpy of transitions were obtained by DSC. Valence state determination and local structure studies were performed using XANES/EXAFS at the Mo-K edge (ESRF, France, Grenoble). The results confirmed the Mo(VI) valence state in Cs 2 MoO 4 , Cs 2 Mo 2 O 7 , Cs 2 Mo 3 O 10. A pre-edge feature [1s(Mo) 4d(Mo)+2p(O)] was also observed, characteristic of tetrahedral MoO 4 symmetry or distorted MoO 6 octahedra. A. L. Smith 1 , E. Epifano 1 , A. Volfi 1 , M. Abbink 1 , L. van Eijck 1 , P. Benigni 2 1 Delft University of Technology, Radiation Science & Technology department, Delft, The Netherlands 2 Aix Marseille Université, IM2NP, UMR CNRS 7334, Marseille, France Cs 2 TeO 4 a b c Intensity (arb. units) 2θ( o C) [1] www.eera-jpnm.eu/inspyre/ [2] M. Tourasse et al., J. Nucl. Mater. 1800 (1992) 49-57 [3] TAF-ID, www.oecd-nea.org/science/taf-id/ [4] A.C. Momin et al., J. Nucl. Mater. 185 (1991) 308-310 Conclusions Using these data as input for CALPHAD thermodynamic models, the composition and amount of formed phases in the JOG can be predicted as a function of oxygen potential and temperature. Contact: Anna L. Smith Radiation Science and Technology department Delft University of Technology Email: [email protected]

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Experimental study of Joint-Oxyde-Gaine (JOG) systems in Fast Neutron Reactors

The JOG is a very-complex multicomponent system, including Cs2MoO4 (major phase), Cs2Te, CsI, Cs2I2, but the exact composition is still not well-known. This work aims to obtain reliable experimental data for this multi-element system and use them to develop thermodynamic models based on the CALPHAD methodology.

Context of the study The present study was performed in the framework of the European INSPYRE project, dedicated to the investigation of the (U,Pu)O2 fuel behaviour under irradiation in Generation-IV Sodium-cooled Fast Reactors (SFRs) and Lead-cooled Fast Reactors (LFRs) [1]. Due to the very high thermal gradients in SFRs and LFRs (~ 450 K·mm-1), the volatile fission products generated during irradiation (e.g. Cs, I, Te, Mo) migrate from the center of the fuel pin (~2300 K) towards the pellet edge (~973 K), and accumulate in the space between fuel and cladding, forming an oxide layer of a few hundred micrometers, the so-called JOG layer (Joint Oxide Gaine) [2].

Lattice parameters evolution with composition and temperature were investigated using X-ray diffraction. The thermal expansion of Cs2TeO4 (αV~107.9·10-6 K-1) is much higher than that of UO2 (αV~32.4·10-6 K-1) [4].

Enthalpies of melting of key compounds were measured using differential scanning calorimetry (DSC) . These differed in some cases quite substantially from computed values in the available CALPHAD model [3].

Study of the Cs-Mo-O system Enthalpies of formation of Cs2Mo2O7 and Cs2Mo3O10 were

determined using solution calorimetry.

Cs2Mo2O7 + n1CsOH = sol. 1 2MoO3 + n2CsOH = sol. 1 Mo + 3/2O2 = MoO3 2Cs + 2H2O = 2CsOH + H2 H2 + 1/2O2 = H2O 2Cs + 2Mo + 7/2O2 = Cs2Mo2O7 ∆𝒇𝒇𝑯𝑯𝒎𝒎 = − 𝟐𝟐𝟐𝟐𝟐𝟐𝟐𝟐.𝟓𝟓 ± 𝟐𝟐.𝟐𝟐 𝒌𝒌𝒌𝒌/𝒎𝒎𝒎𝒎𝒎𝒎

Study of Cs2(Te,Mo)O4 solid solutions Structural investigations were performed using neutron

diffraction at the PEARL beamline. Cs2TeO4 is isostructural with Cs2MoO4, i.e. orthorhombic in space group Pnma.

Phase diagram data in the Cs2TeO4-Cs2MoO4 section and enthalpy of transitions were obtained by DSC.

Valence state determination and local structure studies were performed using XANES/EXAFS at the Mo-K edge (ESRF, France, Grenoble).

The results confirmed the Mo(VI) valence state in Cs2MoO4, Cs2Mo2O7, Cs2Mo3O10. A pre-edge feature [1s(Mo) →4d(Mo)+2p(O)] was also observed, characteristic of tetrahedral MoO4 symmetry or distorted MoO6 octahedra.

A. L. Smith1, E. Epifano1, A. Volfi1, M. Abbink1, L. van Eijck1, P. Benigni2

1 Delft University of Technology, Radiation Science & Technology department, Delft, The Netherlands 2 Aix Marseille Université, IM2NP, UMR CNRS 7334, Marseille, France

Cs2TeO4 a

b c

Inte

nsity

(arb

. uni

ts)

2θ(oC)

[1] www.eera-jpnm.eu/inspyre/ [2] M. Tourasse et al., J. Nucl. Mater. 1800 (1992) 49-57 [3] TAF-ID, www.oecd-nea.org/science/taf-id/ [4] A.C. Momin et al., J. Nucl. Mater. 185 (1991) 308-310

Conclusions Using these data as input for CALPHAD thermodynamic models, the composition and amount of formed phases in the JOG can be predicted as a function of oxygen potential and temperature.

Contact: Anna L. Smith Radiation Science and Technology department

Delft University of Technology Email: [email protected]