Energy Multiplication and Fissile Fuel Breeding Limits of Accelerator-Driven Systems With Uranium and Thorium Targets

dc.authoridcelik, yurdunaz/0000-0002-9211-8510
dc.authorscopusid7102942712
dc.authorscopusid14027391200
dc.authorscopusid54384850100
dc.authorwosidŞahin, Sŭmer/C-6252-2013
dc.contributor.authorSahin, Sumer
dc.contributor.authorŞahin, Sümer
dc.contributor.authorSarer, Basar
dc.contributor.authorCelik, Yurdunaz
dc.contributor.otherDepartment of Mechanical Engineering
dc.date.accessioned2024-07-05T14:31:34Z
dc.date.available2024-07-05T14:31:34Z
dc.date.issued2015
dc.departmentAtılım Universityen_US
dc.department-temp[Sahin, Sumer] ATILIM Univ, Fac Engn, TR-06836 Ankara, Turkey; [Sarer, Basar] Gazi Univ, Fac Sci, TR-06500 Ankara, Turkey; [Celik, Yurdunaz] Gazi Univ, Inst Sci & Technol, TR-06500 Ankara, Turkeyen_US
dc.descriptioncelik, yurdunaz/0000-0002-9211-8510en_US
dc.description.abstractThe study analyses the integral U-233 and Pu-239 breeding rates, neutron multiplication ratio through (n,xn)- and fission-reactions, heat release, energy multiplication and consequently the energy gain factor in infinite size thorium and uranium as breeder material in an accelerator driven systems (ADS), irradiated by a 1-GeV proton source. Energy gain factor has been calculated as M-energy = 1.67, 4.03 and 5.45 for thorium, depleted uranium (100% U-238) and natural uranium, respectively, where the infinite criticality values are k(infinity) = 0.40, 0.752 and 0.816. Fissile fuel material production is calculated as 53 Th-232(n,gamma)U-233, 80.24 and 90.65 U-238(n,gamma)Pu-239 atoms per incident proton, respectively. The neutron spectrum maximum is by similar to 1 MeV. Lower energy neutrons E < 1 MeV have major contribution on fissile fuel material breeding (>97.5%), whereas their share on energy multiplication is negligible (0.2%) for thorium, depleted uranium. Major fission events occur in the energy interval 1MeV < E < 50 MeV. Copyright (C) 2015, Hydrogen Energy Publications, LLC. Published by Elsevier Ltd. All rights reserved.en_US
dc.identifier.citation11
dc.identifier.doi10.1016/j.ijhydene.2015.01.141
dc.identifier.endpage4046en_US
dc.identifier.issn0360-3199
dc.identifier.issn1879-3487
dc.identifier.issue11en_US
dc.identifier.scopus2-s2.0-84926203445
dc.identifier.startpage4037en_US
dc.identifier.urihttps://doi.org/10.1016/j.ijhydene.2015.01.141
dc.identifier.urihttps://hdl.handle.net/20.500.14411/706
dc.identifier.volume40en_US
dc.identifier.wosWOS:000352749500001
dc.identifier.wosqualityQ1
dc.language.isoenen_US
dc.publisherPergamon-elsevier Science Ltden_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectAccelerator driven systemsen_US
dc.subjectThoriumen_US
dc.subjectUraniumen_US
dc.subjectEnergy multiplicationen_US
dc.subjectFissile fuel breedingen_US
dc.subjectNuclear hydrogen productionen_US
dc.titleEnergy Multiplication and Fissile Fuel Breeding Limits of Accelerator-Driven Systems With Uranium and Thorium Targetsen_US
dc.typeArticleen_US
dspace.entity.typePublication
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relation.isAuthorOfPublication.latestForDiscovery565a82c2-51d6-4b83-98c0-f1bcbae75db9
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relation.isOrgUnitOfPublication.latestForDiscoveryf77120c2-230c-4f07-9aae-94376b6c4cbb

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