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Neutronic Analysis for the Effects of High-Level Radioactive Waste Distribution on Subcritical Multiplication Parameters in ADS Reactor Amer A. Al Qaaod a , Volodymyr Gulik b a International Centre for Theoretical Physics (ICTP), Trieste, Italy b


  1. Neutronic Analysis for the Effects of High-Level Radioactive Waste Distribution on Subcritical Multiplication Parameters in ADS Reactor Amer A. Al Qaaod a , Volodymyr Gulik b a International Centre for Theoretical Physics (ICTP), Trieste, Italy b Institute for Nuclear Research, Kyiv, Ukraine 57 th International Winter Meeting on Nuclear Physics, 21-25 January 2019, Bormio, Italy

  2. Motivation Nuclear Waste Transmutation Nuclear Waste Management Strategy Composition of spent nuclear fuel Reduction of Radiological Toxicity by P&T Schematic picture of an accelerator-driven system (ADS) concept

  3. Method Monte Carlo N Particle (MCNP) model and core description Table 1 : ADS reactor core description for two zone model. Description Inner zone Outer Zone Core radius 15 cm 63 cm Core height 126 cm 126 cm No. of fuel elements 392 320 Type of fuel pins WWER-1000 WWER-1000 Coolant Helium/ LBE Graphite Fuel element pitch 1.275 cm 6 cm Radius of pin’s cladding 0.455 cm 0.455 cm Radius of pin’s fuel 0.393 cm 0.393 cm Fuel enrichment 20% 4% Horizontal and vertical cross-section view of MCNPX model for two regions 10.96 g/cm 3 10.96 g/cm 3 Density of the fuel Fuel Cladding material zirconium + 1% zirconium + 1% Niobium Niobium (a) Nonuniform (b) Uniform (c) Spiral Three core models are considered in which selected Plutonium and minor actinide (Pu, Am, and Cm) loaded inside the inner zone

  4. Results  Subcritical multiplication parameters B y using MCNPX we calculated the fission neutrons and source neutrons for the proposed models then we calculated the subcritical multiplication parameters from the following equations:   F 1 (1/ k ) , F S      eff k , M ,   s 1 (1/ k ) F S S s Table 2 : Subcritical multiplication parameters and Pu/ MA Fission Rate (FR) for three core Where, models at fixed k eff = 0.97 M - Neutron multiplication, Φ * M K s Pu/ MA - FR K s - Subcritical multiplication factor, Model Liquid He LB E Liquid He LB E Liquid He LB E Liquid He LB E 7.47 7.82 0.866 0.872 0.200 0.211 0.622 0.653 Uniform Φ * - Neutron source efficiency, 10.59 11.24 0.906 0.911 0.297 0.317 0.634 0.666 Nonuniform F - Total fission neutron 10.08 10.69 0.901 0.906 0.281 0.300 0.619 0.652 Spiral S - Total source neutron  Neutron Spectrum Neutron flux per lethargy (arbitrary unit) Neutron flux per lethargy (arbitrary unit) Neutron flux per lethargy (arbitrary unit) Nonuniform - Liquid Helium coolant Nonuniform - LBE coolant Nonuniform - Liquid Helium coolant Uniform - Liquid Helium coolant Uniform - LBE coolant Nonuniform - LBE coolant Spiral - Liquid Helium coolant 0.01 0.01 Spiral - LBE coolant 0.01 1E-3 1E-3 1E-3 1E-4 1E-4 1E-4 1E-5 1E-5 1E-5 1E-6 1E-6 1E-6 1E-8 1E-6 1E-4 0.01 1 100 1E-8 1E-6 1E-4 0.01 1 100 1E-8 1E-6 1E-4 0.01 1 100 Neutron Energy (MeV) Neutron Energy (MeV) Neutron Energy (MeV) Fig. 4c : Neutron spectrum for the Fig. 4a : Neutron spectrum for the three Fig. 4b : Neutron spectrum for the Nonuniform model with two coolant type models in inner zone in case of Liquid three models in inner zone in case of (Liquid helium and LBE) in inner zone helium coolant LBE coolant

  5. Thank you ou fo for y you our at atte tention For more de details s welco come me to my p poster er

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