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SINBAD ABSTRACT NEA-1553/48

Osaka Nickel Sphere Benchmark Experiment (OKTAVIAN)



1. Name of Experiment:
 ------------------
 Osaka Nickel Sphere Benchmark Experiment (OKTAVIAN) (1983)

2. Purpose and Phenomena Tested:
 ----------------------------
 Neutron leakage spectra from a 32 cm diameter nickel sphere were measured
 between 30 keV and 15 MeV by the time-of-flight technique using a 14 MeV
 D-T neutron generator.

3. Description of the Source and Experimental Configuration:
 --------------------------------------------------------
 A 300 keV Cockcroft-Walton type accelerator, OKTAVIAN of Osaka University
 was used to accelerate deuterons to a kinetic energy of 245 keV. The
 deuteron beam was led through a narrow tube to the centre of a nickel
 sphere where pulsed 14.1 MeV monochromatic neutrons were produced by the
 T(d,n)He-4 fusion reaction. The source strength is angle dependent (see
 Figures 3 and 4). The 32 cm diameter nickel sphere consisted of 99.63% Ni.

4. Measurement System and Uncertainties:
 ------------------------------------
 The detectors used were:

 Detector Diameter Thickness Energy covered
 (cm) (cm) (MeV)
 ---------------------------------------------------------------------
 NE-213 scint. 12.7 5.08 0.03-15

 NE-213 scint. 5.08 5.08 (14) neutron source monitor
 ---------------------------------------------------------------------
 Measurements of neutron spectra were carried out for high energy region
 (between 1 MeV and 15 MeV) and low energy region (30 keV to 15 MeV).
 Energy dependent statistical errors, large below about 0.04 MeV,
 elsewhere 1 - 10%. The uncertainty of the source spectrum in the 14 to
 15 MeV energy range is about 8 %.

5. Description of Results and Analysis:
 -----------------------------------
 Leakage current energy spectrum of neutrons was measured in "absolute values"
 by the time-of-flight technique between 30 keV and 15 MeV, about 9.5 m from
 the sphere centre. The detectors could view the entire surface of the sphere.

 Run-to-run neutron source monitoring was done using NE-213 detector which
 viewed directly the d-t source and was located at 482 cm from the target.

 The experimental configuration is suitable for one-dimensional modelling,
 although for more accurate results an explicit geometrical model including
 source anisotropy, and calculation in time domain is recommended.

 The recommended (semi) 2-D MCNP5(X) input allowing time and energy domain
 analysis is provided in NI2d.i.
 Two older computational models for the MCNP-4B code are also included:
 mcnp1d.inp: simple spherical 1-D model with an isotropic source
 mcnp3d.inp: model including sphere geometry, collimators and source anisotropy

6. Quality assessment:
 -----------------
 The OKTAVIAN NICKEL experiment is of benchmark quality for nuclear data
 validation purposes.

 For detailed evaluation see [8].


7. Author/Organizer
 ----------------
 Experiment and analysis:
 Akito Takahashi,J. Yamamoto, K. Sumita
 Faculty of Nuclear Engineering

 Department of Engineering
 Osaka University
 2-1 Yamadaoka, Suita-shi Osaka-fu, 565 Japan


 T. Kasahara, H. Hashikura, M. Akiyama, Y. Oka, S. Kondo
 Nuclear Engineering Research Laboratory, Faculty of Engineering
 University of Tokyo
 Tokai-mura, Ibaraki 319-11, JAPAN


 Compiler of data for Sinbad:
 I. Kodeli
 OECD/NEA, 12 bd des Iles, 92130 Issy les Moulineaux, France


 Quality assessment:
 A. Milocco, Institut Jožef Stefan, Jamova 39, Ljubljana, Slovenia


 Reviewer of compiled data:
 A. Trkov
 Institute Jozef Stefan, Jamova 39, 1000 Ljubljana, Slovenia


8. Availability:
 ------------
 Unrestricted

9. References:
 ----------
 [1] K. Sumita, A. Takahashi, T. Kasahara, et al: "Measurements of Neutron
 Leakage Spectra from 16 cm Radius Nickel Sphere",
 OKTAVIAN Report A-84-04 (1984)
 [2] A. Takahashi, J. Yamamoto, K. Oshima, et al: "Measurement of Double
 Differential Neutron Emission Cross Sections for Fusion Reactor Candidate Elements",
 Journal of Nuclear Science and Technology, Vol.21, No.8, 577-598 (1984)
 [3] A. Takahashi, J. Yamamoto, H. Hashikura, et al: "Measurement and Analysis
 of Neutron Leakage Spectrum from Nickel Sphere for 14 MeV Neutron Source",
 Journal of Nuclear Science and Technology, Vol.23, No.6, 477-486 (1986)
 [4] A. Takahashi: "Integral Neutronics Experiments at OKTAVIAN",
 OKTAVIAN Report B-83-01 (1983)
 [5] A. Trkov: "Comments on the Oktavian Nickel Sphere Benchmark",
 Institute Jozef Stefan, Ljubljana, Slovenia, IJS-DP-8096, July 1999.
 [6] NEA Nuclear Science Committee: "International Handbook of Evaluated
 Criticality Safety Benchmark Experiments, Nuclear Energy Agency",
 Organisation for Economic Co-operation and Development,
 NEA/NSC/DOC(95)03.
 [7] Yo Makita and Akito Takahashi: "IAEA Benchmark Problem Based on the
 Time-of-Flight Experiment on Nickel Sphere at OKTAVIAN/Osaka University",
 IAEA, http://ripcnt01.iaea.or.at/nds/databases/fendl/FENDL.htm.
 [8] A. Milocco, The Quality Assessment of the OKTAVIAN Benchmark Experiments,
 IJS-DP-10214, April 2009
 [9] A. Milocco, A. Trkov, I. Kodeli: "The OKTAVIAN TOF Experiments in SINBAD:
 Evaluation of the Experimental Uncertainties",
 Annals of Nuclear Energy 37 (2010) pp. 443-449


10. Data and Format:
 ---------------

 DETAILED FILE DESCRIPTIONS
 --------------------------
 Filename          Size[bytes] Content
 ---------------- ----------- -------------
  1 okni-abs.htm    9.712  This information file
  2 okni-exp.htm    30.530 Description of Experiment
  3 Oktavian.pdf 2,934,763 Document describing quality assessment of OKTAVIAN experiments
  4 NI2d.i           2,618 Recommended 2-D MCNP5(X) input allowing time and energy domain analysis
  5 mcnp1d.inp       6.174 1-D MCNP-4B Input (OBSOLETE-cavity & detector modeling approximations)
  6 mcnp3d.inp      18.159 3-D MCNP-4B Input (OBSOLETE-cavity & detector modeling approximations)
  7 Ni-Fig1.tif     67.321 Figure 1: Plan view of the OKTAVIAN facility (high quality)
  8 Ni-Fig2.tif     37.660 Figure 2: View of the experimental arrangement (high quality)
  9 Ni-Fig3.tif     36.441 Figure 3: Angular dependence of the neutron source energy (high quality)
 10 Ni-Fig4.tif     39.377 Figure 4: Angular dependence of the neutron yield (high quality)
 11 Ni-Fig1.gif     14.381 Figure 1: Plan view of the OKTAVIAN facility (preview)
 12 Ni-Fig2.gif      7.514 Figure 2: View of the experimental arrangement (preview)
 13 Ni-Fig3.gif     10.307 Figure 3: Angular dependence of the neutron source energy (preview)
 14 Ni-Fig4.gif      6.019 Figure 4: Angular dependence of the neutron yield (preview)
 15 Ni-Fig5.gif      7.414 Figure 5: Leakage neutron spectrum
 16 Ni-Fig6.gif     12.038 Figure 6: Leakage neutron spectrum
 17 Ni-Fig7.gif      8.384 Figure 7: Source spectra comparison
 18 Ni-Fig8.gif     12.211 Figure 8: Calculated leakage spectrum dependence on the source spectrum
 19 Ni-Fig9.gif     12.415 Figure 9: Calculated leakage spectrum dependence on the geometrical model (1D/3D)
 20 Ni-F10a.gif     11.312 Figure 10a: Calculated spectrum dependence on nuclear data (high energy)-3D model
 21 Ni-F10b.gif     10.899 Figure 10b: Calculated spectrum dependence on nuclear data (low energy)-3D model
 22 OKTNI_2.pdf  1.083.954 Reference
 23 OKTNI_1.pdf    692.505 Reference
 24 OKTNI_3.pdf    647.601 Reference
 25 ane-10.pdf     585,384 Reference


 File OKNI_EXP.HTM contains the following tables:
 A table with the source neutron spectrum, and 2 tables of measured neutron leakage
 spectra (high and low energy range).

 Figures are stored in TIFF format using LZW compression and GIF (preview) format.
 
SINBAD Benchmark Generation Date: 8/2000
SINBAD Benchmark Last Update: 2/2010