Renewability and Sustainability Aspects of Nuclear Energy

dc.authorscopusid7102942712
dc.contributor.authorŞahin, Sümer
dc.contributor.otherDepartment of Mechanical Engineering
dc.date.accessioned2024-07-05T14:26:03Z
dc.date.available2024-07-05T14:26:03Z
dc.date.issued2014
dc.departmentAtılım Universityen_US
dc.department-tempATILIM Univ, Fac Engn, Dept Mech Engn, TR-06836 Ankara, Turkeyen_US
dc.description.abstractRenewability and sustainability aspects of nuclear energy have been presented on the basis of two different technologies: (1) Conventional nuclear technology; CANDU reactors. (2) Emerging nuclear technology; fusion/fission (hybrid) reactors. Reactor grade (RG) plutonium, U-233 fuels and heavy water moderator have given a good combination with respect to neutron economy so that mixed fuel made of (ThO2/RG-PuO2) or (ThC/RG-PuC) has lead to very high burn up grades. Five different mixed fuel have been selected for CANDU reactors composed of 4 % RG-PuO2 + 96 % ThO2; 6 % RG-PuO2 + 94 % ThO2; 10 % RG-PuO2 + 90 % ThO2; 20 % RG-PuO2 + 80 % ThO2; 30 % RG-PuO2 + 70 % ThO2, uniformly taken in each fuel rod in a fuel channel. Corresponding operation lifetimes have been found as similar to 0.65, 1.1, 1.9, 3.5, and 4.8 years and with burn ups of similar to 30 000, 60 000, 100 000, 200 000 and 290 000 MW.d/ton, respectively. Increase of RG-PuO2 fraction in radial direction for the purpose of power flattening in the CANDU fuel bundle has driven the burn up grade to 580 000 MW. d/ton level. A laser fusion driver power of 500 MWth has been investigated to burn the minor actinides (MA) out of the nuclear waste of LWRs. MA have been homogenously dispersed as carbide fuel in form of TRISO particles with volume fractions of 0, 2, 3, 4 and 5 % in the Flibe coolant zone in the blanket surrounding the fusion chamber. Tritium breeding for a continuous operation of the fusion reactor is calculated as TBR = 1.134, 1.286, 1.387, 1.52 and 1.67, respectively. Fission reactions in the MA fuel under high energetic fusion neutrons have lead to the multiplication of the fusion energy by a factor of M = 3.3, 4.6, 6.15 and 8.1 with 2, 3, 4 and 5 % TRISO volume fraction at start up, respectively. Alternatively with thorium, the same fusion driver would produce similar to 160 kg U-233 per year in addition to fission energy production in situ, multiplying the fusion energy by a factor of similar to 1.3.en_US
dc.identifier.citation0
dc.identifier.doi10.1063/1.4895863
dc.identifier.endpage70en_US
dc.identifier.isbn9780735412514
dc.identifier.issn0094-243X
dc.identifier.scopus2-s2.0-84984532223
dc.identifier.scopusqualityQ4
dc.identifier.startpage65en_US
dc.identifier.urihttps://doi.org/10.1063/1.4895863
dc.identifier.urihttps://hdl.handle.net/20.500.14411/92
dc.identifier.volume1615en_US
dc.identifier.wosWOS:000345993100012
dc.language.isoenen_US
dc.publisherAmer inst Physicsen_US
dc.relation.ispartof4th International Conference on Advances in Nuclear Science and Engineering (ICANSE) -- SEP 16-19, 2013 -- Denpasar, INDONESIAen_US
dc.relation.ispartofseriesAIP Conference Proceedings
dc.relation.publicationcategoryKonferans Öğesi - Uluslararası - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subject[No Keyword Available]en_US
dc.titleRenewability and Sustainability Aspects of Nuclear Energyen_US
dc.typeConference Objecten_US
dspace.entity.typePublication
relation.isAuthorOfPublication565a82c2-51d6-4b83-98c0-f1bcbae75db9
relation.isAuthorOfPublication.latestForDiscovery565a82c2-51d6-4b83-98c0-f1bcbae75db9
relation.isOrgUnitOfPublicationf77120c2-230c-4f07-9aae-94376b6c4cbb
relation.isOrgUnitOfPublication.latestForDiscoveryf77120c2-230c-4f07-9aae-94376b6c4cbb

Files

Collections