Energy multiplication and fissile fuel breeding limits of accelerator-driven systems with uranium and thorium targets

dc.contributor.authorŞAHİN, Sümer
dc.contributor.authorŞARER, Başar
dc.contributor.authorÇELİK, Yurdunaz
dc.date.accessioned2022-08-05T12:13:06Z
dc.date.available2022-08-05T12:13:06Z
dc.date.issued2015-01-25
dc.description.abstractThe study analyses the integral 233U and 239Pu 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 Menergy ¼ 1.67, 4.03 and 5.45 for thorium, depleted uranium (100% 238U) and natural uranium, respectively, where the infinite criticality values are k∞ ¼ 0.40, 0.752 and 0.816. Fissile fuel material production is calculated as 53 232Th(n,g) 233U, 80.24 and 90.65 238U(n,g) 239Pu atoms per incident proton, respectively. The neutron spectrum maximum is by ~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.
dc.identifier.urihttp://hdl.handle.net/20.500.11905/1504
dc.language.isoen
dc.publisherInternational Journal of Hydrogen Energy
dc.subjectenergy systems engineering
dc.titleEnergy multiplication and fissile fuel breeding limits of accelerator-driven systems with uranium and thorium targets
dc.typeArticle
dspace.entity.type

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