Nature of the coolant (steam-rich or steam-poor) given by different steam flow rate.
Material composition of the control rod (Ag-In-Cd or B4C).
Sump pH and thermal-hydraulic conditions imposed (evaporating or not)
Fuel temperature (350-3100°C), cumulated hydrogen production (0 - 0.12 kg), molten mass (0 - 2.0 kg), caesium and iodine relative release from the core, caesium and iodine relative released mass into the containment , iodine aerosol concentration (0 - 0.1 g/m3), iodine absorved on wet condenser (0 - 0.001 mol)
ATHLET-CD
COCOSYS
ASTEC/IODE
IMPAIR3-JRC
INSPECT
MELCOR
SCDAP/RELAP5
ICARE2
ASTEC/SOPHAEROS
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2013, Pages 4-10,
https://doi.org/10.1016/j.anucene.2013.03.037.
[2] L. Tiborcz, S. Beck, «Uncertainty and sensitivity analysis of the fission product behaviour in the Phébus FPT1 test with the system code AC2», Nuclear Engineering and Design, Volume 429, 2024, 113594,
https://doi.org/10.1016/j.nucengdes.2024.113594.
[3] N. Girault et al., «LWR severe accident simulation: Iodine behaviour in FPT2 experiment and advances on containment iodine chemistry», Nuclear Engineering and Design, Volume 243, 2012, Pages 371-392,
https://doi.org/10.1016/j.nucengdes.2011.11.011.
[4] K. Mueller et al., «Final interpretation report of the PHEBUS test FPT0 (bundle aspects)», DG JRC Institute for energy, October 2007.
[5] N. Girault et al., Towards a better understanding of iodine chemistry in RCS of nuclear reactors, Nuclear Engineering and Design 239 (2009) 1162–1170. doi:10.1016/j.nucengdes.2009.02.008
[6] FPT0, FPT1 and FPT2 final reports.
[7] Cousin et al. Modelling of fission-product transport in the reactor coolant system. Annals of Nuclear Energy 61 (2013) 135–142.
https://doi.org/10.1016/j.anucene.2013.02.035
[8] B. Xerri et al., «Ab initio calculations and iodine kinetic modeling in the reactor coolant system of a pressurized water reactor in case of severe nuclear accident», Computational and Theoretical Chemistry,
Volume 990, Pages 194-208, 2012,
https://doi.org/10.1016/j.comptc.2012.02.024