NEA-1860 IFPE/IFA-519.9.
IFPE/IFA-519.9, Three PWR rods irradiated to 90 MWd/kg UO2
NAME OF EXPERIMENT, COMPUTER, DESCRIPTION OF EXPERIMENT, STATUS, REFERENCES, LANGUAGE, NAME AND ESTABLISHMENT OF AUTHORS, MATERIAL, CATEGORIES
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| Program name | Package id | Status | Status date |
|---|---|---|---|
| IFPE/IFA-519.9 | NEA-1860/01 | Arrived | 12-OCT-2011 |
Machines used:
| Package ID | Orig. computer | Test computer |
|---|---|---|
| NEA-1860/01 | Many Computers |
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3. DESCRIPTION OF EXPERIMENT
Three rods were irradiated in IFA-429 to approximately 26-29 MWd/kgUO2 were instrumented with bellows type pressure transducers for monitoring in-pile fission gas release by measuring the rod internal pressure. They were irradiated in the Halden rig IFA-519.9.
Rod DC was irradiated in the upper cluster and rods DH and DK were irradiated in the lower cluster of this assembly in IFA-429. The average linear heat rate during the irradiation was below 20kW/m. At this low power, fission gas was accumulated within the matrix without perceptible release. This was confirmed during re-instrumentation since no change in pressure was measurable from the initial fill pressure. The burn-up archived at the end of IFA-429 was approximately 28.7 MWd/kgUO2 for rod DC, 25.9 MWd/kgUO2 for rod DH, and 28.9 MWd/kgUO2 for rod DK.
The rods in IFA-519.9 were re-instrumented with bellows type pressure transducers so that fission gas release could be monitored from measurements of the rod internal pressure during irradiation. However, In-pile data were only available for rods DH and DK because the fission gas release could not be monitored for rod DC since there has been no open connection between the instrumented part with the pressure transducer and the fuel stack. Rods had different combinations of the grain size and the pellet-cladding gap to compare the difference in behaviour of the three rods. They were irradiated at a power level of around 40kW/m and the burn-up archived at the end of IFA-519.9 was performed approximately 90MWd/kgUO2.
After irradiation in IFA-519.9, PIE was performed on rods DC, DH and DK at Kjeller to obtain information on the effect of the design parameters on fission product distribution, fission gas release and dimensional changes causing PCMI. Rod DC was punctured both in the instrumentation and in the fuel rod plenum.
Three rods were irradiated in IFA-429 to approximately 26-29 MWd/kgUO2 were instrumented with bellows type pressure transducers for monitoring in-pile fission gas release by measuring the rod internal pressure. They were irradiated in the Halden rig IFA-519.9.
Rod DC was irradiated in the upper cluster and rods DH and DK were irradiated in the lower cluster of this assembly in IFA-429. The average linear heat rate during the irradiation was below 20kW/m. At this low power, fission gas was accumulated within the matrix without perceptible release. This was confirmed during re-instrumentation since no change in pressure was measurable from the initial fill pressure. The burn-up archived at the end of IFA-429 was approximately 28.7 MWd/kgUO2 for rod DC, 25.9 MWd/kgUO2 for rod DH, and 28.9 MWd/kgUO2 for rod DK.
The rods in IFA-519.9 were re-instrumented with bellows type pressure transducers so that fission gas release could be monitored from measurements of the rod internal pressure during irradiation. However, In-pile data were only available for rods DH and DK because the fission gas release could not be monitored for rod DC since there has been no open connection between the instrumented part with the pressure transducer and the fuel stack. Rods had different combinations of the grain size and the pellet-cladding gap to compare the difference in behaviour of the three rods. They were irradiated at a power level of around 40kW/m and the burn-up archived at the end of IFA-519.9 was performed approximately 90MWd/kgUO2.
After irradiation in IFA-519.9, PIE was performed on rods DC, DH and DK at Kjeller to obtain information on the effect of the design parameters on fission product distribution, fission gas release and dimensional changes causing PCMI. Rod DC was punctured both in the instrumentation and in the fuel rod plenum.
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10. REFERENCES
- K. Lassmann, J. van de Laar:
A new Data-Condensation Method based on Multidimensional Minimisation, Technical Report JRC-ITU-TN-2001/32, 2001
- K. LASSMANN and J. van de LAAR:
"A new Data-Condensation Method Based on Multidimensional Minimisation", KERNTECHNIK 69 (2004) 21-25
- K. Lassmann, J. van de Laar:
A new Data-Condensation Method based on Multidimensional Minimisation, Technical Report JRC-ITU-TN-2001/32, 2001
- K. LASSMANN and J. van de LAAR:
"A new Data-Condensation Method Based on Multidimensional Minimisation", KERNTECHNIK 69 (2004) 21-25
NEA-1860/01, included references:
- J.A. Turnbull:Concluding report on three PWR rods irradiated to 90 MWd/kgUO2 in IFA519.9:
Analysis of measurements obtained in-pile and by PIE (Documentation - HWR-668,
January 2001)
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NEA-1860/01
429-SUM.txt Summary of base irradiation in IFA-429 IFA-519.9-Summary.pdf Description of the irradiation
PRE-CHAR-519-9.txt Pre-characterization data
IFA-429-BASE-HIST-DC.DAT Base irradiation histories in IFA-429, rod DC
IFA-429-BASE-HIST-DH.DAT Base irradiation histories in IFA-429, rod DH
IFA-429-BASE-HIST-DK.DAT Base irradiation histories in IFA-429, rod DK
IFA-519.9-HIST-DC.DAT Base irradiation histories in IFA-519.9, rod DC
IFA-519.9-HIST-DH.DAT Base irradiation histories in IFA-519.9, rod DH
IFA-519.9-HIST-DK.DAT Base irradiation histories in IFA-519.9, rod DK
519.9-TFDB.dat Full (uncondensed) irradiation history of IFA-519-9
519.9-TFDB-varlist.txt Variables included in the data file 519-9-TFDB.dat
IFA-519-9-PIE.txt Description of the irradiation
README-519-9.TXT Readme
IFA-519.9-QAREP.pdf QA report
HWR-668.pdf Electronic report
fig1-429-profiles.pdf IFA-429: Axial power distribution figure
Keywords: burnup, diffusion, experimental data, fission gas release, fuels, modelling, post-irradiation examination.