1944-20 Joint ICTP-IAEA Workshop on Nuclear Reaction Data for...
Transcript of 1944-20 Joint ICTP-IAEA Workshop on Nuclear Reaction Data for...
1944-20
Joint ICTP-IAEA Workshop on Nuclear Reaction Data for AdvancedReactor Technologies
BORELLA Alessandro
19 - 30 May 2008
Institute For Reference Materials and MeasurmentsEC JRC IRMMRetiesweg 111B-2440 Geel
BELGIUM
Cross Section Measurements and Uncertainties of Cross Section Data.
Monte Carlo methodsEUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Simple Monte Carlo Example
Evaluate G=jg(x)dx, with g(x) = V i -
Simulation approach:"darts game"For k = 1,...,N: choose i ^ yk randomly in (0r1):
it x^+v= < 1 r tally a "hit"
number of hitsG = [area under curve] - (1 1) N
EUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Monte Carlo approach to particle transport- Random Numbers are generated to solve particle transport- Vs. deterministic codes
- Relies on:• Physics and particle transport equations• Data (cross sections) for the various process
• Where data are not available relies on models
- The history are tracked by generating random number (RN):so-called "random walks"
- According to the value of the RN, the XS and the physics, the particlefate will be different
- The source particle and possible secondary particles are tracked inthe medium according to the geometry and composition
- Quantities of interested (the so-called tallies) are computed
- More info and documentation: http://mcnp-green.lanl.gov/
MCNP/MCNPXEUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
MCNP is a code developed by LANL to simulatethe transport of neutrons, gamma rays andelectrons by the Monte Carlo method. Itsimulates a coupled transport, i.e., it alsoaccounts for transport of secondary particleresulting the interaction of primary particles.
MCNPX extends the capacilties of MCNP to otherparticles (e.g. charged particles, heavy ions,pions etc.)
Jnli Problems that can be solved *-ttiEUROPEAN COMMISSION ,,,,,.,J,,L
Malerials and Measure me nlsWorkshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Problems that can be solved/Fields of application* Reactor calculations
BurnupCriticality
* Medical applicationRadiography
* Detectore.g. C6D6
* High energy physics (MCNPX)* Space applications
EUROPEAN COMMISSIONMCNP users groups
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Application
Medical (BNC T. proton therapy, etc.)
Spacecraft, Cosmic Rays, SEE. propulsion
Detectors, experiment1;. Threat Reduction
ATW, .ADS. Energy Amplifier:
Fuel cycles, beginning to end. including storage
Accelerator Shielding ami Health Physics
Theoretical Physics
Neutron Production for Scattering
Isotope Production
Radiography
MCNFXMCNP code development
Homeland Security
Material*; stadies (IFMIF)
Radioactive Ion Benin1;
Irradiation Facilities
Neutrino Targets
Light Source1;, electron machines
U Groups
50
4:
39
3"
32
28
23
21
14
12
11
ID
6
•*
4
4
3
Percent
1?
12
11
11
9
8
-r
6
4
4
3
3
i
1
1
1
1
EUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Examples- Gamma ray transport- Neutron transport
Structure of the input file- Cell- Surfaces- Materials (XS)- Source definition- Tally- Additional options
Output files- Binary- Out file- Other files (mctal)
Tallies examplesEUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
F l ; Surface Current
F2: S u rface F Luence
FA: CellFLuence
F5: Detector FLuenoe
Ene igy Deposit ion
F7: Fission Energy Deposition
FS: Pulse Height
JRCEUROPEAN COMMISSION
Example 1 - gamma transport mWorkshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Institute for ReferenceMaterials and Mea s u re me r>ls
Point source in (0,0,0)Isotropic source
Ey = 1 MeV
Response in a sphereDeposited energyRin=10 cm Rout=15 cm
BaF
EUROPEAN COMMISSIONExample 1 - gamma transport m
Institute for Reference.Marerials and Measurenicnls
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
JRCEUROPEAN COMMISSION
Example 1 - gamma transport mInstitute for Reference.Marerials and Measurenicnls
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
EUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
example 1: g source response for c6d6cc —1 02 13 0c
-1.0020-20 10-10
imp:n,p,e=0imp:n,p,e=1imp:n,p,e=1
$ univers$ univers$ univers
cc surface definitions for PM10 so 10.0 $ global univers20 so 15.0 $ global universc
cMODE P Ecc ZZAAA AT1 ZZAAA AT2M1 6012 0.5 1002 0.496 1001 0.004 $ c6d6cSDEF ERG=1 PAR=2 POS=0 0 0ccF8 : P E 2E8' ' 0 999I 1.0 $ 1 keV/bincNPS 1e5
EUROPEAN COMMISSIONExample 1 - c6d6 result
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
EUROPEAN COMMISSIONExample 1 - BaF2 result
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
JRCEUROPEAN COMMISSION
Example 3 - neutron transport mWorkshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Institute for ReferenceMaterials and Mea s u re me r>ls
Point source in (0,0,0)Isotropic source
En = 0.1-1 MeV
Flux in a sphere vs EFlux through surfacesRin=10 cm Rout=10.5 cm
Co+Ag
cp(E) spectrum ?
EUROPEAN COMMISSION
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
example 1: n transport response for co+ag
c —1 02 13 04 0
-8.9030-20 10-1020 -30
imp:n,p,e=0imp:n,p,e=1imp:n,p,e=1
imp:n,p,e=1
$ univers$ univers$ univers
$ univers
c surface definitions for PM10 so 10.0 $ global univers20 so 10.5 $ global univers30 so 100.0
cMODE NMl 27059 1.0 $ CocSDEF ERG=D1 PAR=1 POS=0 0 0SI1 H .1 1SP1 0 1cF12:n 30 $surface flux 2T12 1.0e00 999I 1.0e03 $ 10 ns binscNPS 1e07
JRCEUROPEAN COMMISSION
Example 3 - flux attenuation by co+agWorkshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
1.00E-08 -
8.00E-09 -
6.00E-09 --
4.00E-09 --
2.00E-09 -
0.00E+00
•ArmmInstitute for Reference.Marerials and Measurenicnls
1.00E-04 2.00E-04 3.00E-04 4.00E-04 5.00E-04 6.00E-04 7.00E-04 8.00E-04 9.00E-04 1.00E-03
En / MeV
JRCEUROPEAN COMMISSION
Example 2 - neutron transport mWorkshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
Institute for ReferenceMaterials and Mea s u re me r>ls
Point source in (0,0,0)Isotropic source
En = 1 MeV
Flux in a sphere vs EFlux through surfacesRin=10 cm Rout=50 cm
H2O
EUROPEAN COMMISSIONExample 2 - flux through surfaces m
Institute tor ReferenceMaterials and Measurement
Workshop On Nuclear Data for Advanced Reactor Technologies, ICTP 22-05-2008, A. Borella
100000
10000
1000
100
10
1 n
0.1 n
0.01 n
c^ 1E-3 -;
^ 1E-4 -j
1E-5
1E-6
1E-7
1E-8
1E-9
CD
1E-101E
i i i i i i i i i
10 1E-9 1E-8 1E-7 1E-6 1E-5 1E-4 1E-3 0.01 0.1• • • • I
10
E /MeVn