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dc.contributor.authorOrtiz, Nestor Rubenen_US
dc.contributor.authorRickard, I. C. Massachusetts Institute of Technologyen_US
dc.contributor.authorDriscoll, Michael J.en_US
dc.contributor.authorRasmussen, Norman C.en_US
dc.contributor.otherMassachusetts Institute of Technology. Department of Nuclear Engineeringen_US
dc.contributor.otherUnited States. Department of Energyen_US
dc.contributor.otherU.S. Atomic Energy Commissionen_US
dc.date.accessioned2014-09-16T23:32:10Z
dc.date.available2014-09-16T23:32:10Z
dc.date.issued1972en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/89707
dc.description"May, 1972."en_US
dc.descriptionAlso issued as an Sc. D. thesis by the first author and supervised by the third and fourth author, MIT Dept. of Nuclear Engineering, 1972en_US
dc.descriptionIncludes bibliographical references (pages 223-225)en_US
dc.description.abstractU.S. Atomic Energy Commission contracten_US
dc.description.abstractThe energy spectrum of the neutron flux in a realistic mockup of the blanket region of a large liquid-metal-cooled fast breeder reactor was measured using three different spectrometers: He-3 and Li-6 semiconductor detectors and a Proton-Recoil proportional counter. The He-3 detector was operated in the sum and difference modes, and the Li-6 detector in the sum, difference and triton modes. The experimental data was unfolded using direct, integral and derivative techniques. Methods were developed or perfected to enable use of the He-3 detector over the neutron energy range from 10 keV to 1.3 MeV and the Li-6 detector from 10 keV to 3.1 MeV; the Proton-Recoil detector was operated in the region from 2 keV to 1.5 MeV. In general, good agreement was found between the experimental measurements for all detector types, modes of operation and methods of unfolding, except for the low-energy He-3 data. The present experimental results and previously reported data obtained using a method based on gamma line broadening are in relatively good agreement in the high energy region above 0.8 MeV. The measured neutron spectrum is also similar in shape to neutron spectra measured at ANL in critical assembly mockups of large LMFBR cores, but systematically softer, as expected.. However, there is a large discrepancy in the energy region from 10 keV to 50 keV between the present results and either spectra unfolded from foil data or those numerically calculated using the 1-D ANISN code in the S8 option with 26 energy groups.en_US
dc.format.extent225 pagesen_US
dc.publisherCambridge, Mass. : Massachusetts Institute of Technology, Dept. of Nuclear Engineering, [1972]en_US
dc.relation.ispartofseriesMITNE ; no. 129en_US
dc.relation.ispartofseriesCOO (Series) ; 3060-3en_US
dc.relation.ispartofseriesAEC research and development reporten_US
dc.subject.lccTK9008.M41 N96 no.129en_US
dc.subject.lcshLiquid metal fast breeder reactorsen_US
dc.subject.lcshLiquid metal cooled reactorsen_US
dc.subject.lcshNeutron fluxen_US
dc.titleInstrumental methods for neutron spectroscopy in the MIT blanket test facilityen_US
dc.typeTechnical Reporten_US
dc.identifier.oclc856653117en_US


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