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Benchmark analysis of Iron Cross- sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux, Nov. 27-28, 2013
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Page 1: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

Benchmark analysis of Iron Cross-sections

I. Kodeli (JSI, Ljubljana, Slovenia)

EFFDOC-1221

JEFF Meeting, NEA- Issy-les-Moulineaux, Nov. 27-28, 2013

Page 2: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

2

SINBAD - Radiation Shielding Experiments

Scope and Objectives • Compilation of high quality experiments for validation

and benchmarking of computer codes and nuclear data used for radiation transport and shielding problems encompassing:

reactor shielding, PV dosimetry (46)

fusion blanket neutronics (31)

accelerator shielding (23)

• Low and inter-mediate energy particles applications.

• Contains 100 experiments • Distribution on CD-ROM by the RSICC and the NEA DB.

http://www.nea.fr/html/science/shielding/sinbad/sinbadis.htm

http://www-rsicc.ornl.gov/BENCHMARKS.html

sinbadis.htm

Page 3: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

Quality Assessment of Fusion and Accelerator Shielding Benchmarks

• Since the experimental data presently available in SINBAD are of varying quality, a revision and classification of the benchmark experiments according to the completeness and reliability of information is being undertaken in order to provide users with easier choices and help them make better use of the experimental information.

• A series of 45 experiments, mostly of relevance for fusion neutronics and accelerator shields were revised and updated SINBAD compilations released (2008-2013);

• Calculation should be able to reproduce the experiment as exactly as reasonably possible, avoiding unnecessary approximations;

• Compare calculations to pure measured data. Often ‘processed’ measured data are referred to as ‘measured’;

• Description of the experiment should not be mixed with the benchmark model. The description of the experiment, the details, the uncertainties of physical parameters (geometry, material), the procedure to derive data (unfolding) are the bases for the judgment of the benchmark quality.

Page 4: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

SINBAD: Re-evaluated Fe Benchmarks

SINBAD Benchmark / quality Additional information needed on; (new data)

OKTAVIAN Fe ~ ♦♦♦ or ♦♦ very large uncertainties of the measurements

FNS Iron dogleg-duct ♦♦ neutron source spectrum, detector response function

TUD Iron slab ~ ♦♦♦ neutron source, pulse height spectrum

FNG Stainless Steel ~ ♦♦♦ A comprehensive geometry description would be helpful

FNG ITER Dose Rate ♦♦♦ /

FNG/TUD ITER Bulk ~ ♦♦♦ n &g flux uncertainties, original pulse-height distributions

FNG ITER Bulk ♦♦♦ /

IPPE-Fe , 14 MeV n source (new 2D & 3D MCNP5 models prepared)

JANUS phase I ♦♦♦ & VIII ♦♦♦

ASPIS NESDIP 2 ♦/♦♦ & 3 ♦♦♦ neutron source spectrum approximations

Ispra Iron ♦♦ Geometry model details and approximations, background ?

ISIS 800 MeV protons (120cm

Concrete & 60cm Iron) ~ ♦♦♦

(new MCNPX model prepared)

HIMAC 400 MeV/nucleon C ions

on Fe shield ~ ♦♦♦

large measurement uncertainties, unfolding uncertainty and

parameter uncertainties needed (new PHITS model

prepared)

TIARA 43 & 68 MeV Protons ♦♦♦

Page 5: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

IMPROVEMENTS

– more experimental information from literature

– refinement of the D-T source model

– experimental source spectra simulations

– new MCNP5/X models

– Sensitivity studies (neutron source description,

composition, geometry where available)

Page 6: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

Fe-56(n,inel) from JEFF-3.1

NEW MEASUREMENTS

– RPI (Yaron Danon):

high resolution

transmission

measurements;

– GEEL (Arjan Plompen)

inelastic cross-section

measurements.

Page 7: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

IPPE Fe sphere # 1 (4.5 cm): C & E compared to XS uncertainties

0

2

4

6

8

10

0 2 4 6 8 10 12 14 16

0.01

0.1

IPPE-Fe sphere #1

Ne

utr

on s

pectr

a /

Me

V

Energy (MeV)

Exp. sph.#1

MCNP5

0.1 1

2

4

6

8

10

0.1 10.01

0.1

IPPE-Fe sphere #1

Ne

utr

on s

pectr

a /

Me

V

Energy (MeV)

Exp. sph.#1

MCNP5

Err

or

(%)

0.1 1 10

2

4

6

8

10

0.1 1 10

0.01

0.1

IPPE-Fe sphere #1

Neutr

on s

pectr

a /

MeV

Energy (MeV)

Exp. sph.#1

MCNP5

XS uncertainty

Uncert

ain

ty (

%)

Page 8: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

0.1 1

0

2

4

6

8

10

12

14

0.1 1

0.01

0.1

1

IPPE-Fe sphere #5

Leakag

e s

pectr

a (

n/M

eV

)

Energy (MeV)

Exp. sph.#5

MCNP5

Err

or

(%)

0

5

10

15

2 4 6 8 10 12 14 16

1E-3

0.01

IPPE-Fe sphere #5

Lea

ka

ge

sp

ectr

a (

n/M

eV

)

Energy (MeV)

Exp. sph.#5

MCNP5

XS uncertainties

Un

cert

ain

ty (

%)

IPPE Fe sphere # 5 (30cm): C&E compared to XS uncertainties

0.1 1 10

0

5

10

15

0.1 1 10

1E-3

0.01

0.1

1

IPPE-Fe sphere #5

Leakag

e s

pectr

a (

n/M

eV

)

Energy (MeV)

Exp. sph.#5

MCNP5

XS uncertainties

Uncert

ain

ty (

%)

Explicit modelisation of the collimator and

providing TOF spectra and collimator-detector

system detailed geometry would allow to

compare MCNP results directly with the

measured TOA spectra, without needing any

response function, nor TOA-Energy

transformation.

Page 9: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

--------------------------------------------------------------------------------

SINBAD Index – Reactor Shielding --------------------------------------------------------------------------------

• Winfrith Iron Benchmark (ASPIS)

• Winfrith Iron 88 Benchmark (ASPIS)

• Winfrith Water/Iron Benchmark (ASPIS-PCA REPLICA)

• Winfrith Neutron-Gamma Ray Transport through Water/Steel Arrays (ASPIS)

• NESDIP-2 Benchmark (ASPIS)

• NESDIP-3 Benchmark (ASPIS)

• JANUS Phase I (Neutron Transport Through Mild and Stainless Steel)

• JANUS Phase VIII (Neutron Transport Through Sodium Mild Steel)

• Ispra Iron Benchmark (EURACOS)

• Karlsruhe Iron Sphere

• Wuerenlingen Iron Benchmark (PROTEUS)

• Gamma Production X-Sections from Thermal Neutron Capture in 14 elements & SS

• Gamma Production X-Sections from Fast Neutron Capture in 14 elements & SS

• ORNL TSF Iron Broomstick

• ORNL TSF Stainless Steel Broomstick

• ORNL Neutron Transport Through Iron and SS - Part I

• University of Illinois Iron Sphere (CF-252)

• University of Tokyo-YAYOI Iron Slab

• Snezynsk Photon Leakage Spectra from Al, Ti, Fe, Cu, Zr, Pb, U238 Spheres

• NAÏADE 1 Iron Benchmark (60cm)

Page 10: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

--------------------------------------------------------------------------------

SINBAD Index – FUSION --------------------------------------------------------------------------------

• Osaka Iron Sphere (OKTAVIAN)

• FNG-SS Shield (integral measurements)

• FNG-ITER Blanket Bulk Shield (integral measurements)

• FNG/TUD ITER Blanket Bulk Shield (spectra)

• FNG-ITER Dose Rate Experiment

• TUD Iron Slab Experiment

• IPPE Iron Shells

• ORNL 14-MeV Neutron SS/B Poly Slab

• University of Illinois Iron Sphere (D-T)

--------------------------------------------------------------------------------

SINBAD Index – Accelerator Shielding --------------------------------------------------------------------------------

• Neutron Production from Thick Targets of C, Fe, Cu, Pb by 30- and 52-MeV p+

• TIARA 40 & 65 MeV Neutron Transmission Through Iron, Concrete & Polyethylene

• ROESTI I, II and III (CERN)

• HIMAC High energy Neutron (<800 MeV) Measurements in Iron

• ISIS Deep-Penetration Neutrons through Concrete & Fe Shields using p-800 MeV

Page 11: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

IRPhEP, ICSBEP databases

Approved evaluations stored in IRPhE and/or ICSBEP:

• ALARM-CF-FE-SHIELD-001 Neutron and Photon Leakage Spectra from CF-252 Source at Center of Six Iron Sphere of Different Diameters, Gennady Manturov, Yevgeniy Rozhikhin, and Lev Trykov (Institute of Physics and Power Engineering – Russian Federation).

ICSBEP fast critical benchmarks with Fe used as reflector and/or cladding are sensitive to FE inelastic XS and could be useful for validation.

Page 12: Benchmark analysis of Iron Cross- sections€¦ · Benchmark analysis of Iron Cross-sections I. Kodeli (JSI, Ljubljana, Slovenia) EFFDOC-1221 JEFF Meeting, NEA- Issy-les-Moulineaux,

• The SINBAD database currently contains compilations and evaluations of

experiments for 46 reactor shielding problems, 31 for fusion neutronics

shielding and 23 for accelerator shielding cases.

• 25 benchmarks include Iron or steel as shielding material.

• Since the experimental data presently available in SINBAD are of varying

quality, a revision and classification of the benchmark experiments

according to the completeness and reliability of information is being

undertaken in order to identify missing information and facilitate the

choice and make better use of the experimental information. A series of

45 experiments of relevance for fission, fusion neutronics and for

accelerator shields were already revised and reclassified.

• Several fast critical and Alarm system benchmarks from ICSBEP are

relevant for Fe benchmarking.

Conclusions


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