nuclear data uncertainty propagation using a total …€¦ · · 2018-03-09nuclear data...
TRANSCRIPT
Nuclear data uncertainty propagation using a Total Monte Carlo approach
Arjan Koningamp and Dimitri RochmanNRG Petten The Netherlands
ampUniv Uppsala
Workshop on Uncertainty Propagation in the Nuclear Fuel Cycle
April 24-25 2013 Uppsala Sweden
2
Europe by night
Petten
3
Petten site
httpwwwnrgeu
4
Complete infrastructure in Petten
fabrication recycling material
irradiation in HFR
post irradiation examination inhot cell laboratories
Actinide lab
(~10 in the world)
Large Test Reactor
(~10 in the world)
Hot Cells
(~20 in the world)
And we combine this with nuclear computational simulations
5
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
2
Europe by night
Petten
3
Petten site
httpwwwnrgeu
4
Complete infrastructure in Petten
fabrication recycling material
irradiation in HFR
post irradiation examination inhot cell laboratories
Actinide lab
(~10 in the world)
Large Test Reactor
(~10 in the world)
Hot Cells
(~20 in the world)
And we combine this with nuclear computational simulations
5
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
3
Petten site
httpwwwnrgeu
4
Complete infrastructure in Petten
fabrication recycling material
irradiation in HFR
post irradiation examination inhot cell laboratories
Actinide lab
(~10 in the world)
Large Test Reactor
(~10 in the world)
Hot Cells
(~20 in the world)
And we combine this with nuclear computational simulations
5
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
4
Complete infrastructure in Petten
fabrication recycling material
irradiation in HFR
post irradiation examination inhot cell laboratories
Actinide lab
(~10 in the world)
Large Test Reactor
(~10 in the world)
Hot Cells
(~20 in the world)
And we combine this with nuclear computational simulations
5
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
And we combine this with nuclear computational simulations
5
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
6
Contents
bull Introductionbull Full control over nuclear data + uncertainty propagation +
reactor calculations ndash 4 stages1 Create the best possible nuclear data library TENDL2 Validate TENDL against integral experiments and
benchmarks3 Perform Total Monte Carlo around the central values of
TENDL for uncertainty propagation in reactor analyses4 Generalize Total Monte Carlo methodology to full core
analysesbull Conclusions
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Automating nuclear science
7
- Use (extremely) robust software- Store all human intelligence in input files and scripts- Rely on reproducibility and quality assurance
Road to success
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Strategy
1 Create the best possible nuclear data library (TENDL) usingbull Experimental data (EXFOR database)bull The TALYS nuclear model codebull Resonance information (TARES code)bull Pick and choose from existing nuclear data libraries (ENDFB-VII
JEFF etc)2 Validate TENDL against open-source integral experiments and
benchmarksbull ICSBEP criticality benchmarksbull SINBAD shielding benchmarksbull IRPHE reactor benchmarksbull Activation and decay heat experiments
This establishes the central values ie a ldquonormalrdquo nuclear data library
8
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Strategy
3 Randomize nuclear data around the central values of TENDL to perform Total Monte Carlobull Obtain exact uncertainties for criticality benchmarks etcbull Perform reactorburnup calculations on pin cell and assembly
level including uncertaintiesbull The lsquoPetten Methodrsquo Monte Carlo optimization of nuclear data
4 Generalize TMC methodology to full core calculationsbull Generate random nuclear data libraries for PANTHER CASMO-
SIMULATE RELAP etcbull Perform dynamical calculations transient and thermohydraulics
including uncertainties
If 1-4 are successful we have the best central nuclear data values andthe most flexible and exact uncertainty methodology
9
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Safety and sustainability ndash nuclear data
Starting point basic nuclear data forreactor and fuel cycle analyses have uncertainties
Required insight in how uncertaintyof nuclear data is propagated tonuclear energy safety and sustainability issues
Observation the world is workinghard to yield answers to this within 10-20 years
Claim it can be done faster than thatusing TALYS
Measurements plusmnuncertainty
TALYS Download TALYS-14wwwtalyseu
Nuclear data
Reactor physicscode (MCNPetc)
Staticalreactor behavior
Transientcode
Dynamicalreactor behavior
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
11
TALYS Evaluated Nuclear Data Library TENDL-2012
bull Neutron proton deuteron triton helium-3 alpha and gamma data librariesbull 2430 targets (all isotopes with lifetime gt 1 sec)bull Complete reaction description in ENDF-6 format MF1-MF40 up to 200 MeVbull MCNP-libraries (ldquoACE-filesrdquo) PENDF files and multi-group covariance data
Default Global calculations by TALYS-148 and TARES (resonances)
which are overruled by
Adjusted TALYS calculations (340 input files) and Resonance Atlas-based TARES calculations
which are overruled by
TALYS-normalization to ~200 (experimental) evaluated reaction channels from other libraries (eg IRDFF light nuclides main channels of 235238U 239Pu)
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
12
TALYS
bull Nuclear model code by NRG Petten CEA-BRC UL Bruxellesbull (Almost) Complete nuclear reaction input and outputReleasebull wwwtalyseubull Latest official version TALYS-14 released december 23 2011Software issuesbull Most used nuclear reaction code in the worldbull Very flexible in use robust and readable consistent programmingbull 300 page manual 20 widely varying sample casesbull TALYS open source
bull 600-800 users worldwide who give valuable feedbackbull Nuclear data software around TALYS (ie the step to technology)
NRG proprietary
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
13
General 5Nuclear
models 46
High energy models and exps 149
Data libs and low energy exps 193
Fusion 31
Medical 90
Astrophysics 101
0
020406080
100120140160180
2003 2004 2005 2006 2007 2008 2009 2010 2011 2012
TALYS publications
publications
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Nuclear data libraries for nuclear technology
14
ldquoThe TALYSTENDL system has rapidly evolved to be a likely candidate to form the basis for a single global evaluated nuclear data library system hellip In the event that TALYSTENDL continues to emerge as an unchallenged global contender it is recommended that the IAEA provide moral and other support helliprdquo
Ken Kozier AECL IAEA meeting on long-term data needs 2011
E Sartori Nuclear data for radioactive waste management Ann Nuc En (2013)
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
15
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
16
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
High Fidelity Resonances (HFR)
17
URR derived resonance ladders
GOE for each (jl)
Wigner law for spacing
KD03 OMP foraverage parameters
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
HFR
D Rochman AJ Koning J Kopecky J-C Sublet P Ribonand M Moxon ``From average parameters to statisticalresolved resonances Ann Nuc En 51 60 (2013)
18
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
TENDL nuclear data library
19
AJ Koning and D Rochman Modern nuclear data evaluation with the TALYS code systemldquoNuclear Data Sheets 113 2841 (2012)
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Testing TENDL - Criticality safety ICSBEP
20
International Criticality Safety Benchmark Evaluation Project516 evaluations 4405 cases (2010 DVD)
Type of fissile materialLEU IEU HEU MIX PU 233U
Physical form of fissile materialCompound Metal SolutionMiscellaneous
Neutron spectrumThermal intermediate fast mixed
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Criticality safety leu-comp-therm
21
TCA Valduc
(S van der Marck ND-2013)
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Criticality safety Na
22
ZPR
6-6a
ZPR
6-7
ZPR
6-7
hig
h 24
0 Pu
ZPR
3-48
ZPR
3-56
Ni Δρsim500 pcm240Pu ~300 pcm
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Shielding benchmarks
23
OktavianLiF Al Si Ti Cr Mn Co Cu Zr Mo W
FNSBe C N O Fe Pb5 angles
LLNLLi Be C N O Mg Al Ti Fe Pb D2O H2Oconcrete polyethylene teflon
NISTH2O Cd
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Shielding example LLNL Mg 07 mfp
24
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
25
ldquoTotalrdquo Monte Carlo
bull Propagating covariance data is an approximation of true uncertaintypropagation (especially regarding ENDF-6 format limitations)
bull Covariance data requires extra processing and ldquosatellite softwarerdquo forapplication codes
bull Alternative Create an ENDF-6 file for each random sample and finish the entire physics-to-application loop (Koning and Rochman Ann NucEn 35 2024 (2008)
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Automating nuclear reactions Total Monte Carlo
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
37
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
38
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
39
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
40
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
41
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
42
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
43
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
44
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
45
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
46
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
47
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
48
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
49
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
50
TMC Application criticality benchmarks
Total of 60000 random ENDF-6 files
Sometimes deviation from Gaussian shape
D Rochman AJ Koning and SC van der Marck``Uncertainties for criticality-safety benchmarks and keff distributions Ann Nuc En 36 810-831 (2009)
Yields uncertainties on benchmarks
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Pu239 cross sections + uncertainties
51
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
52
Optimization of Pu-239
bull Select 120 ICSBEP benchmarksbull Create 630 random Pu-239 libraries all within or closely
around the uncertainty bandsbull Do a total of 120 x 630 =75600 MCNP criticality
calculationsbull Do another 120 x 4 calculations
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
53
Optimization of Pu-239
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
54
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
55
SFR void coefficient
bull KALIMER-600 Sodium Fast Reactor (Korea)bull Total Monte Carlo with MCNPbull Uncertainties due to Na D Rochman et al NIM A612 374
(2010)
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
D Rochman AJ Koning and SC van der Marck ``Exact nuclear data uncertainty propagation for fusion design Fusion Engineering and Design 85 669-682 (2010)
56
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
57Calculate uncertainties in inventory with Serpent
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
58
PWR burn-up calculations
D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
- Slide Number 32
- Slide Number 33
- Slide Number 34
- Slide Number 35
- Slide Number 36
- Slide Number 37
- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Publications
Getrsquom all at ftpftpnrgeupubwwwtalysbib_koningpublicationshtmlExamplesbull DF da Cruz D Rochman and AJ Koning ``Uncertainty analysis on reactivity and discharged
inventory due to U235238 Pu239240241 and fission products nuclear data uncertainties -application to a pressurized water reactor fuel assembly to be published (2013)
bull D Rochman AJ Koning J Kopecky J-C Sublet P Ribon and M Moxon ``From averageparameters to statistical resolved resonances Ann Nuc En 51 60 (2013)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation with the TALYS code system Nucl Data Sheets 113 2841 (2012)
bull D Rochman and AJ Koning ``Random adjustment of the H in H2O neutron thermal scattering data Nucl Sci Eng 172 no 3 287-299 (2012)
bull D Rochman AJ Koning and D da Cruz ``Propagation of 235236238U and 239Pu nuclear data uncertainties for a typical PWR fuel element Nuclear Technology 179 no 3 323-338 (2012)
bull AJ Koning and D Rochman ``Modern nuclear data evaluation Straight from nuclear physics toapplications Journ Kor Phys Soc 59 no 23 773 (2011)
bull D Rochman and AJ Koning ``How to randomly evaluate nuclear data a new method applied toPu-239 Nucl Sci Eng 169(1) 68 (2011)
bull D Rochman AJ Koning SC van der Marck A Hogenbirk and CM Sciolla ``Nuclear data uncertainty propagation Perturbation vs Monte Carlo Ann Nuc En 38 942 (2011)
bull D Rochman AJ Koning DF da Cruz ``Uncertainties for the Kalimer Sodium Fast Reactor voidcoefficient keff Beff burn-up and radiotoxicity Jap Journ Sci Techn 48 (8) 1193 (2011)
59
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
- Slide Number 28
- Slide Number 29
- Slide Number 30
- Slide Number 31
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- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-
Conclusions
bull By simultaneously developing and maintaining1 A complete modern nuclear data library TENDL2 An unprecedented integral validation scheme with integral
experiments and benchmarks3 A Total Monte Carlo method applied on well-established
Monte Carlo and deterministic reactor codes 4 An extension to full core analyses
complete probability distributions (uncertainties covariances) for many reactor and inventory quantities of interest can be obtainedbull Total Monte Carlo If we can calculate it once we can also
calculate it 1000 times randomly varying the inputbull Safety uncertainty risk and money are equivalent also in the
nuclear world Therefore exact uncertainty propagation will be beneficial
60
- Nuclear data uncertainty propagation using a Total Monte Carlo approach
- Europe by night
- Petten site
- Complete infrastructure in Petten
- Slide Number 5
- Contents
- Automating nuclear science
- Strategy
- Strategy
- Safety and sustainability ndash nuclear data
- TALYS Evaluated Nuclear Data Library TENDL-2012
- TALYS
- Slide Number 13
- Nuclear data libraries for nuclear technology
- Slide Number 15
- Slide Number 16
- High Fidelity Resonances (HFR)
- HFR
- TENDL nuclear data library
- Testing TENDL - Criticality safety ICSBEP
- Criticality safety leu-comp-therm
- Criticality safety Na
- Shielding benchmarks
- Shielding example LLNL Mg 07 mfp
- ldquoTotalrdquo Monte Carlo
- Automating nuclear reactions Total Monte Carlo
- Slide Number 27
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- Slide Number 38
- Slide Number 39
- Slide Number 40
- Slide Number 41
- Slide Number 42
- Slide Number 43
- Slide Number 44
- Slide Number 45
- Slide Number 46
- Slide Number 47
- Slide Number 48
- Slide Number 49
- TMC Application criticality benchmarks
- Pu239 cross sections + uncertainties
- Optimization of Pu-239
- Optimization of Pu-239
- Slide Number 54
- SFR void coefficient
- TMC for fusion Optimized Cu6365 file vs Oktavian integral performance
- Slide Number 57
- Slide Number 58
- Publications
- Conclusions
-