simulation of spallation and transmutation minor actinides in fast subcritical reactor
DESCRIPTION
Simulation of spallation and transmutation minor actinides in fast subcritical reactor. J OINT I NSTITUTE FOR N UCLEAR R ESEARCH. apprentice: Przemysław Stanisław Stanisz supervisor: Aleksander Polański (LIT). DUBNA 29.07.2011. Models and Codes Used for Simulations. - PowerPoint PPT PresentationTRANSCRIPT
Simulation of spallation and transmutation minor actinides
in fast subcritical reactor
JOINT INSTITUTE FOR NUCLEAR RESEARCH
DUBNA 29.07.2011
apprentice: Przemysław Stanisław Staniszsupervisor: Aleksander Polański (LIT)
Models and Codes Used for Simulations
MCNP (Monte Carlo N-Particle code) is developed by Los Alamos National Lab (LANL) to
simulate the transport of neutrons, gamma rays and electrons by the Monte Carlo method. It simulates a coupled transport, i.e., it also accounts for transport of secondary particle resulting the interaction of primary particles.
MCNPX (Monte Carlo N-Particle eXtended) extends the capacilties of MCNP to other particles (e.g.
charged particles, heavy ions, pions etc.) CINDER90 code and library to developed for the description of
nuclide inventories produced in a wide range of radiation environments
The Spallation Proces
Fast Direct Process:- Intra-Nuclear Cascade (nucleon-nucleon collisions)
Compound Nuclei:- Evaporation (mostly neutrons)
- High-Energy Fissions
Spallation Neutron Yield
Spallation Neutron Yield (mean multiplicity of emitted neutrons)
The number of emitted neutrons varies as a function of the target nuclei and the energy of the incident particle
L. Pienkowski, F. Goldenbaum, D. Hilscher, U. JahnkeNeutron multiplicity distributions for 1.94 to 5 GeV/c proton-, antiproton-, pion-, kaon-,and deuteron-induced spallation reactions on thin and thick targets
Spallation Neutron Spectrum
The spectrum of spallation neutrons evaporated from an excited heavy nucleus bombarded by high energy particles is similar to the fission neutron spectrum but shifts a little to higher energy
Spallation Product Distribution
The spallation product distribution varies as a function of the target material and incident proton energy. It has a very characteristic shape:
ADS geometry modelCharacteristics Destription
MeV 1000 protons, beam power 1,16MW
Thermal fission power 100MW
Diameter of the core. 520 [mm]
Height of a fuel active part 630 [mm]
Radius of lead reflector 520 [mm]
Number of the fuel elements in assembles
18
Number of fuel assembles 133
Maximal gain factor Keff=0,97
Heat-carrier helium
Radius of concrete shielding 190 [cm]
Max neutron flux 6.64E15 [cm2/s]
FAST Reactor geometry modelCharacteristics Destription
Thermal fission power 100MW
Diameter of the core. 520 [mm]
Height of a fuel active part
780 [mm]
Radius of lead reflector 520 mm
Number of the fuel elements in assembles
18
Number of fuel assembles
153
Maximal gain factor Keff=1,1
Heat-carrier helium
Radius of concrete shielding
190 cm
Max neutron flux 6.64E15 [cm2/s]
Reactivity change in burnup cycle
ADS and Fast Reactor Neutron Spectra
Mass evolution of Plutonium
0.00E+005.00E+011.00E+021.50E+022.00E+022.50E+021.10E+02
1.20E+02
1.30E+02
1.40E+02
1.50E+02
1.60E+02
1.70E+02
1.80E+02
1.90E+02
Transmutation of Pu239
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+00 5.00E+01 1.00E+02 1.50E+02 2.00E+02 2.50E+027.60E+01
7.70E+01
7.80E+01
7.90E+01
8.00E+01
8.10E+01
8.20E+01
8.30E+01
8.40E+01Transmutation of Pu240
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+005.00E+01
1.00E+021.50E+02
2.00E+022.50E+02
2.50E+01
3.00E+01
3.50E+01
4.00E+01
4.50E+01
5.00E+01
Transmutation of Pu241
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+00 5.00E+01 1.00E+02 1.50E+02 2.00E+02 2.50E+022.64E+01
2.66E+01
2.68E+01
2.70E+01
2.72E+01
2.74E+01
2.76E+01
2.78E+01
Transmutation of Pu242
Burnup [GWd/MTU]
Mas
s [g
]
Mass evolution of Minor Actinide (MA)
0.00E+00 1.00E+02 2.00E+021.40E+01
1.50E+01
1.60E+01
1.70E+01
1.80E+01
1.90E+01
2.00E+01
2.10E+01
Transmutation of Np237
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+00 1.00E+02 2.00E+028.50E+00
9.00E+00
9.50E+00
1.00E+01
1.05E+01
1.10E+01
1.15E+01
Transmutation of Am 241
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+00 1.00E+02 2.00E+027.00E+00
7.20E+00
7.40E+00
7.60E+00
7.80E+00
8.00E+00
8.20E+00
8.40E+00
Transmutation of Am243
Burnup [GWd/MTU]
Mas
s [g
]0.00E+00 1.00E+02 2.00E+02
2.70E+002.90E+00
3.10E+00
3.30E+00
3.50E+00
3.70E+00
3.90E+00
4.10E+004.30E+00
4.50E+00
Transmutation of Cm244
Burnup [GWd/MTU]
Mas
s [g
]
0.00E+00 1.00E+02 2.00E+022.50E-01
3.00E-01
3.50E-01
4.00E-01
4.50E-01
5.00E-01
Transmutation of Cm245
Burnup [GWd/MTU]
Mas
s [g
]
Thank you
for attention