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Oxide phase characterization in simulated high burn-up
UO_2 fuels in the early stages of a nuclear severe
accident
C. Le Gall, E. Geiger, O. Proux, M. Rovezzi, P.L. Solari, M. Hunault, V.
Klosek, C. Riglet Martial, J. Léchelle, F. Audubert, et al.
To cite this version:
C. Le Gall, E. Geiger, O. Proux, M. Rovezzi, P.L. Solari, et al.. Oxide phase characterization in simulated high burn-up UO_2 fuels in the early stages of a nuclear severe accident. The 2018 MRS Spring Meeting & Exhibit, Apr 2018, Phoenix, United States. �cea-02338951�
Oxide phase characterization in
simulated high burn-up UO
2
fuels in
the early stages of a nuclear severe
accident
April 2-6, 2018 – Phoenix, Arizona
MRS Spring Meeting 2018
|
Claire Le Gall
CEA Cadarache
|
DEN
|
DEC
|
SA3E
|
LAMIR
C. Le Gall
1, E. Geiger
2, O. Proux
3, M. Rovezzi
3, P.L. Solari
4, M. Hunault
4, V.
Klosek
1, C. Riglet-Martial
1, J. Léchelle
1, F. Audubert
1, Y. Pontillon
1,
J.-L. Hazemann
51CEA / DEN / DEC, 2 DCCE / RMC Canada, 3OSUG-UGA, 4MARS / SOLEIL Synchrotron, 5Institut Néel / CNRS UGA
MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
NUCLEAR FUEL FISSION
Fission products
| PAGE 2 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
D. Heinze Ph.D thesis (2010)
Mo Ba
Fission yield: FP most probably producted
Fission occurs in nuclear fuel pellets
UO2 or (U,Pu)O2 fuel in its Zr alloyed cladding
Pressurized Water Reactor (PWR) Fuel assembly
SEVERE ACCIDENT PHENOMENA
Source term
| PAGE 3 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
Source Term
Nature and quantity of
released radioactive
materials
FP
FP release from the
fuel
J. P. Van Dorsselaere et al., NED 236 (2006) B. R. Sehgal, Nuclear safety in LWR (2012)
Corium formation
Loss of coolant
Cladding
oxidation
BaMoO
4(s)Oxide phase
STUDY OF FPs BEHAVIOR
Mechanism suggested in the literature
| PAGE 4 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
G. Nicaise, 8th International Conference on Candu Fuel (2003) G. Nicaise, NT DPAM/SEMIC 2004/37 (2004)
E. Geiger, PhD thesis (2016) H. Kleykamp, J. Nucl. Mater. (1985)
MoO
2(g)MoO
2(s)MoO
2(g)BaZrO
3(s) Oxide phaseZr
(s)ZrO
2(s)BaO
(s)BaZrO
3(s)BaO
(g)Ba
(g)Mo/Ru
(s)Mo
(g)Mo/Ru
(s)Oxidation
plateau
(1100-1500°C)
High temp.
plateau
(≥ 2300°C)
Temperature
ramp
(400-1100°C)
Temperature
ramp
(1500-2000°C)
Initial State
SIMFuels
SIMFuels SAMPLES
Fabrication data
| PAGE 5 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
Depleted UO
2
+ 11 oxides
(FPs surrogates)
Sintering at 1650°C
during 2h under pure H
2
Elements
Ba
Ce
La
Mo
Sr
Y
Zr
Rh
Pd
Ru
Nd
Concentration
(at%)
0,26
0,61
0,20
0,51
0,13
0,06
0,60
0,03
0,42
0,64
0,91
Concentrations representative of an irradiated fuel
SIMFuels SAMPLES
Thermal treatments
| PAGE 6 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
Mo (s ) + R u(s) + Pd(s) + Rh (s) + ZrO 2 (s) + BaZrO 3(s) + UO2(s) Ru(s) + Pd (s) + Rh(s) + ZrO 2(s) + Ba ZrO3 (s) + MoO2 (s) + UO2(s) Ru(s) + Pd(s) + Rh(s) + ZrO2(s) + BaMo O 4(s) + MoO2 (s) + U O 2(s) ZrO2(s) + BaM oO4(s) + MoO 2 (s) + U4 O9(s2 )
Pd(liq) + MoO2(s) + ZrO2(s)
Pd(liq) + UO2(s) + Ru(s) + Pd(s) + Rh(s ) + + Rh(s) + Ru(s) + UO2(s)
Ru(s) + Mo(s) + Rh3U(s)
H2O/ H2 = 50 H2O/H2 = 0.0 2 Pd (l iq ) + R h (s ) + R u (s ) + M o (s ) + Z rO 2 (s ) + B a Z rO 3 (s ) + U O2 (s ) BaZrO 3(s) BaMo O4(s) Ba - O2 - Mo - Zr - Ru - Rh - Pd - U Temperature (°C) R T ln p (O 2 ) ( k J/ m ol O 2 ) 400 600 800 1000 1200 1400 1600 1800 2000 -500 -450 -400 -350 -300 -250 -200 -150 Mo (s ) + R u(s) + Pd(s) + Rh (s) + ZrO2(s) + Ba ZrO3 (s) + UO2(s) Ru(s) + Pd (s) + Rh(s) + ZrO 2(s) + Ba ZrO3(s) + Mo O2(s) + UO 2(s) Ru(s) + Pd(s) + Rh(s) + ZrO2(s) + BaMo O 4(s) + MoO2 (s) + U O 2(s) ZrO2(s) + BaMo O 4(s) + M oO 2(s) + U4O9(s2 )
Pd(liq) + MoO2(s) + ZrO2(s)
Pd(liq) + UO2(s) +
Ru(s) + Pd(s) + R
h(s) +
+ Rh(s) + Ru(s) + UO2(s)
Ru(s) + Mo(s) + Rh3U(s)
H2O/ H2 = 50 H2O/H2 = 0.0 2 Pd (l iq ) + R h (s ) + R u (s ) + M o (s ) + Z rO 2 (s ) + B a Z rO 3 (s ) + U O 2 (s ) BaZrO 3(s) BaMo O4(s) Ba - O2 - Mo - Zr - Ru - Rh - Pd - U Temperature (°C) R T ln p (O 2 ) ( k J/ m ol O 2 ) 400 600 800 1000 1200 1400 1600 1800 2000 -500 -450 -400 -350 -300 -250 -200 -150 R1700 R1000 R900 R700 R400 O1000 O900 O700 O400
BaZrO
3(s)+ MoO
2(s)+ ½O
2(g)BaMoO
4(s)+ ZrO
2(s)(Ba+Sr)/Mo ≈ 1
(Ba+Sr)/Zr ≈ 0.6
O/Zr ≈ 4
CHARACTERIZATIONS
SEM-EDX
| PAGE 7 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018C. Thouzellier internship (2017), H. Kleykamp, J. Nucl. Mater. (1985); E. Geiger et al. ERMSAR proceedings (2015); E Geiger et al. J. Nucl. Mater. (accepted)
Sample as sintered
1000°C, -292 kJ.mol
-11700°C, -426 kJ.mol
-1O/Zr ≈ 2
(Sr+Ba)/Zr ≈ 1
O/Zr ≈ 2.5
Ba
0,8Sr
0,2ZrO
3ZrO
2Ba
0,9Sr
0,1ZrO
3Mo
Oxide
phase
O/Mo ≈ 5
Ba
0,8Sr
0,2ZrO
3ZrO
2(Ba, Sr)(Zr, Mo)O
xCHARACTERIZATIONS
SEM-EDX
| PAGE 8 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
C. Thouzellier internship (2017), H. Kleykamp, J. Nucl. Mater. (1985); E. Geiger et al. ERMSAR proceedings (2015); E Geiger et al. J. Nucl. Mater. (accepted)
Sample as sintered
1000°C, -292 kJ.mol
-11700°C, -426 kJ.mol
-1O/Mo ≈ 2
Oxide
phase
Metallic
phase
100% Mo
100% Mo
100% Mo
MoO
20 1 2 3 4
5
6 7 8 910
11 19975 20025 20075N
orm(
E)
Energy (eV)
0 1 2 3 4 5 6 78
9 10 11 12 19975 20025 20075 Norm( E ) Energy (eV) R1700 T0 SrMoO4 BaMoO4 MoO3 O1000 O900 T0 MoO2 Mo SrMoO4 BaMoO4 MoO3 MoO2 Mo 0 1 2 3 45
6 7 8 910
11 19975 20025 20075N
orm(
E)
Energy (eV)
0 1 2 3 4 5 6 78
9 10 11 12 19975 20025 20075 Norm( E ) Energy (eV) R1700 T0 SrMoO4 BaMoO4 MoO3 O1000 O900 T0 MoO2 Mo SrMoO4 BaMoO4 MoO3 MoO2 MoCHARACTERIZATIONS
X-ray Absorption Spectroscopy at Mo K-edge
| PAGE 9 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
No strong evolution of Mo
XANES reducing conditions
Metallic Mo
0 1 2 3 45
6 7 8 910
11 19975 20025 20075N
orm(
E)
Energy (eV)
0 1 2 3 4 5 6 78
9 10 11 12 19975 20025 20075 Norm( E ) Energy (eV) R1700 T0 SrMoO4 BaMoO4 MoO3 O1000 O900 T0 MoO2 Mo SrMoO4 BaMoO4 MoO3 MoO2 MoEvolution of Mo local
environment from 900°C in
oxidizing conditions
Consistent with Mo oxidation,
MoO
2formation and the oxide
0 1 2 3 4 5 6 7 8 9 10 17975 18025 18075 Norm( E ) Energy (eV) 0 1 2 3 4 5 6
7
8 9 17975 18025 18075 Norm (E) Energy (eV) BaZrO3 ZrO2 R1700 T0 Zr BaZrO3 ZrO2 Zr O1000 T0 0 1 2 3 4 5 6 7 8 9 10 17975 18025 18075 Norm( E ) Energy (eV) 0 1 2 3 4 5 67
8 9 17975 18025 18075 Norm (E) Energy (eV) BaZrO3 ZrO2 R1700 T0 BaZrO3 ZrO2 O1000 T0 0 1 2 3 4 5 6 7 8 9 10 17975 18025 18075 Norm( E ) Energy (eV) 0 1 2 3 4 5 67
8 9 17975 18025 18075 Norm (E) Energy (eV) BaZrO3 ZrO2 R1700 T0 BaZrO3 ZrO2 O1000 T0 | PAGE 10 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018Zr XANES evolution at 1700°C
in reducing conditions
Consistent with the
continuous BaZrO
3formation and stabilization
0 1 2 3 4 5 6 7 8 9 10 17975 18025 18075 Norm( E ) Energy (eV) 0 1 2 3 4 5 6
7
8 9 17975 18025 18075 Norm (E) Energy (eV) BaZrO3 ZrO2 R1700 T0 Zr BaZrO3 ZrO2 Zr O1000 T0 0 1 2 3 4 5 6 7 8 9 10 17975 18025 18075 Norm( E ) Energy (eV) 0 1 2 3 4 5 67
8 9 17975 18025 18075 Norm (E) Energy (eV) BaZrO3 ZrO2 R1700 T0 BaZrO3 ZrO2 O1000 T0Zr XANES evolution from
1000°C in oxidizing conditions
Destruction of part of the
BaZrO
3phase and formation of
ZrO
2?
Consistent with the oxide phase
evolution (Mo reacts with Ba)
CHARACTERIZATIONS
0 5 10 15 20 25 5 220 5 250 5 280 5 310 5 340 Norm (E ) Energy (eV) BaMoO4 BaZrO3 BaCO3 BaO 1700°C, 10-27 0 5 10 15 20 25 5 220 5 250 5 280 5 310 5 340 Norm (E ) Energy (eV) BaMoO4 BaZrO3 BaCO3 BaO 1700°C, 10-27 | PAGE 11 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018
No Ba XANES evolution at
1700°C in reducing conditions
BaZrO
3XANES analyses of the
O-samples scheduled in April
2018
CHARACTERIZATIONS
HERFD-XANES at Ba L
3-edge
BaZrO3 BaMoO4 BaCO3 BaO R1700 T0BaZrO
3(s) Oxide phaseBaZrO
3(s)ZrO
2(s)Mo/Ru
(s)Mo/Ru
(s)BaMoO
4(s) Oxide phase | PAGE 12 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018MoO
2(g)ZrO
2(s)BaZrO
3(s)Mo/Ru
(s)1000°C
400°C – 900°C
1700°C
Initial State
CONCLUSIONS
Evolution of the oxide phase
Oxidizing atmosphere Reducing atmosphere
ZrO
2(s)To be confirmed
ESRF:
P. Colomp, O. Proux, M. Rovezzi, J. L. Hazemann
MARS/SOLEIL:
M. Hunault, P. L. Solari
CEA/LLCC:
C. Riglet Martial, D. Drouan, C. Tanguy, V. Klosek, J. Léchelle, G. Jomard
CEA/LCU:
F. Garel, P. Matheron, N. Tarisien, X. Itlis, H. Rouquette, J. Raynal,
J. Lamontagne
CEA/LAMIR:
C. Thouzellier, J.C. Richaud, M. Pontillon, G. Volle, A. Gallais During, Y.
Pontillon, F. Audubert, I. Moysan
Commissariat à l’énergie atomique et aux énergies alternatives Centre de Cadarache| 13108 Saint Paul lez Durance T. +33 (0)4 42 25 70 00
Etablissement public à caractère industriel et commercial | R.C.S Paris B 775 685 019 MRS Spring Meeting 2018, Phoenix, Arizona,
| PAGE 14 MRS Spring Meeting 2018, Phoenix, Arizona, April 2-6, 2018