Fission gas production in reactor fuels including the effects of ternary fission

▶ Noble gas productions were simulated in three different nuclear fuels. ▶ Ternary fission was added into CINDER’90 to track ternary fissioned helium. ▶ Xe has by far the largest production, 136Xe decreases with higher fuel enrichment. ▶ Pu based fuel produces less Kr than U based fuel. ▶ Helium pro...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Nuclear engineering and design 2010-11, Vol.240 (11), p.3751-3757
Hauptverfasser: Hu, Jianwei, Hayes, A.C., Wilson, W.B., Rizwan-uddin
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 3757
container_issue 11
container_start_page 3751
container_title Nuclear engineering and design
container_volume 240
creator Hu, Jianwei
Hayes, A.C.
Wilson, W.B.
Rizwan-uddin
description ▶ Noble gas productions were simulated in three different nuclear fuels. ▶ Ternary fission was added into CINDER’90 to track ternary fissioned helium. ▶ Xe has by far the largest production, 136Xe decreases with higher fuel enrichment. ▶ Pu based fuel produces less Kr than U based fuel. ▶ Helium produced mainly from transuranic isotopes. An understanding of gas bubble formation and migration in nuclear fuel and its impacts on fuel and cladding materials requires knowledge of the isotopic composition of the gases and their generation rates. In this paper, we present results of simulations for the production of the dominant noble gases (helium, xenon, krypton) in nuclear fuels for different reactor core configurations and fuel compositions. The calculations were performed using detailed nuclear burn simulations with Monte Carlo nuclear transport, and included ternary fission to ensure an accurate treatment of helium production. For all reactor designs and fuels considered xenon was found to be the most dominant gas produced. Variation in the composition of fission gases is quantified for: (1) the burn time, (2) the composition of the fuel, and (3) the neutron energy spectrum. These three factors determine the relative fraction of each gas and its transmutation into or from stable gas by subsequent neutron capture.
doi_str_mv 10.1016/j.nucengdes.2010.08.020
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_849440847</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0029549310005364</els_id><sourcerecordid>849440847</sourcerecordid><originalsourceid>FETCH-LOGICAL-c377t-b6c9b4564e60cb3cb5a968be8c06b7b410d3e94d2240d8132f46050dd272e06c3</originalsourceid><addsrcrecordid>eNqFkE9vFDEMxSMEEkvbz0AuiNMsniTzJ8eqooBUCQ5U4hZlHGfJapop8QwS375ZbdUrvli23vOzfkK8b2HfQtt_Ou7zhpQPgXivoG5h3IOCV2LXjoNqhs7-ei12AMo2nbH6rXjHfIRTWbUTP24Tc1qyPHiWj2UJG66nMWVZyOO6FBk3mrkucN5Cyge5_iZJMRKuLJcoVyrZl38yng9dijfRz0xXz_1C3N9-_nnztbn7_uXbzfVdg3oY1mbq0U6m6w31gJPGqfO2HycaEfppmEwLQZM1QSkDYWy1iqaHDkJQgyLoUV-Ij-e79ek_G_HqHhIjzbPPtGzsRmONgdEMVTmclVgW5kLRPZb0UF92LbgTQnd0LwjdCaGD0VWE1fnhOcMz-jkWnzHxi11pA9pqVXXXZ10FRX8TFceYKCOFVComF5b036wnsqqMJg</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>849440847</pqid></control><display><type>article</type><title>Fission gas production in reactor fuels including the effects of ternary fission</title><source>ScienceDirect Journals (5 years ago - present)</source><creator>Hu, Jianwei ; Hayes, A.C. ; Wilson, W.B. ; Rizwan-uddin</creator><creatorcontrib>Hu, Jianwei ; Hayes, A.C. ; Wilson, W.B. ; Rizwan-uddin</creatorcontrib><description>▶ Noble gas productions were simulated in three different nuclear fuels. ▶ Ternary fission was added into CINDER’90 to track ternary fissioned helium. ▶ Xe has by far the largest production, 136Xe decreases with higher fuel enrichment. ▶ Pu based fuel produces less Kr than U based fuel. ▶ Helium produced mainly from transuranic isotopes. An understanding of gas bubble formation and migration in nuclear fuel and its impacts on fuel and cladding materials requires knowledge of the isotopic composition of the gases and their generation rates. In this paper, we present results of simulations for the production of the dominant noble gases (helium, xenon, krypton) in nuclear fuels for different reactor core configurations and fuel compositions. The calculations were performed using detailed nuclear burn simulations with Monte Carlo nuclear transport, and included ternary fission to ensure an accurate treatment of helium production. For all reactor designs and fuels considered xenon was found to be the most dominant gas produced. Variation in the composition of fission gases is quantified for: (1) the burn time, (2) the composition of the fuel, and (3) the neutron energy spectrum. These three factors determine the relative fraction of each gas and its transmutation into or from stable gas by subsequent neutron capture.</description><identifier>ISSN: 0029-5493</identifier><identifier>EISSN: 1872-759X</identifier><identifier>DOI: 10.1016/j.nucengdes.2010.08.020</identifier><identifier>CODEN: NEDEAU</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>Applied sciences ; Controled nuclear fusion plants ; Energy ; Energy. Thermal use of fuels ; Exact sciences and technology ; Fission nuclear power plants ; Fuels ; Installations for energy generation and conversion: thermal and electrical energy ; Nuclear fuels ; Preparation and processing of nuclear fuels</subject><ispartof>Nuclear engineering and design, 2010-11, Vol.240 (11), p.3751-3757</ispartof><rights>2010</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c377t-b6c9b4564e60cb3cb5a968be8c06b7b410d3e94d2240d8132f46050dd272e06c3</citedby><cites>FETCH-LOGICAL-c377t-b6c9b4564e60cb3cb5a968be8c06b7b410d3e94d2240d8132f46050dd272e06c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.nucengdes.2010.08.020$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=23403932$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Hu, Jianwei</creatorcontrib><creatorcontrib>Hayes, A.C.</creatorcontrib><creatorcontrib>Wilson, W.B.</creatorcontrib><creatorcontrib>Rizwan-uddin</creatorcontrib><title>Fission gas production in reactor fuels including the effects of ternary fission</title><title>Nuclear engineering and design</title><description>▶ Noble gas productions were simulated in three different nuclear fuels. ▶ Ternary fission was added into CINDER’90 to track ternary fissioned helium. ▶ Xe has by far the largest production, 136Xe decreases with higher fuel enrichment. ▶ Pu based fuel produces less Kr than U based fuel. ▶ Helium produced mainly from transuranic isotopes. An understanding of gas bubble formation and migration in nuclear fuel and its impacts on fuel and cladding materials requires knowledge of the isotopic composition of the gases and their generation rates. In this paper, we present results of simulations for the production of the dominant noble gases (helium, xenon, krypton) in nuclear fuels for different reactor core configurations and fuel compositions. The calculations were performed using detailed nuclear burn simulations with Monte Carlo nuclear transport, and included ternary fission to ensure an accurate treatment of helium production. For all reactor designs and fuels considered xenon was found to be the most dominant gas produced. Variation in the composition of fission gases is quantified for: (1) the burn time, (2) the composition of the fuel, and (3) the neutron energy spectrum. These three factors determine the relative fraction of each gas and its transmutation into or from stable gas by subsequent neutron capture.</description><subject>Applied sciences</subject><subject>Controled nuclear fusion plants</subject><subject>Energy</subject><subject>Energy. Thermal use of fuels</subject><subject>Exact sciences and technology</subject><subject>Fission nuclear power plants</subject><subject>Fuels</subject><subject>Installations for energy generation and conversion: thermal and electrical energy</subject><subject>Nuclear fuels</subject><subject>Preparation and processing of nuclear fuels</subject><issn>0029-5493</issn><issn>1872-759X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqFkE9vFDEMxSMEEkvbz0AuiNMsniTzJ8eqooBUCQ5U4hZlHGfJapop8QwS375ZbdUrvli23vOzfkK8b2HfQtt_Ou7zhpQPgXivoG5h3IOCV2LXjoNqhs7-ei12AMo2nbH6rXjHfIRTWbUTP24Tc1qyPHiWj2UJG66nMWVZyOO6FBk3mrkucN5Cyge5_iZJMRKuLJcoVyrZl38yng9dijfRz0xXz_1C3N9-_nnztbn7_uXbzfVdg3oY1mbq0U6m6w31gJPGqfO2HycaEfppmEwLQZM1QSkDYWy1iqaHDkJQgyLoUV-Ij-e79ek_G_HqHhIjzbPPtGzsRmONgdEMVTmclVgW5kLRPZb0UF92LbgTQnd0LwjdCaGD0VWE1fnhOcMz-jkWnzHxi11pA9pqVXXXZ10FRX8TFceYKCOFVComF5b036wnsqqMJg</recordid><startdate>20101101</startdate><enddate>20101101</enddate><creator>Hu, Jianwei</creator><creator>Hayes, A.C.</creator><creator>Wilson, W.B.</creator><creator>Rizwan-uddin</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SU</scope><scope>7TB</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20101101</creationdate><title>Fission gas production in reactor fuels including the effects of ternary fission</title><author>Hu, Jianwei ; Hayes, A.C. ; Wilson, W.B. ; Rizwan-uddin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c377t-b6c9b4564e60cb3cb5a968be8c06b7b410d3e94d2240d8132f46050dd272e06c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Applied sciences</topic><topic>Controled nuclear fusion plants</topic><topic>Energy</topic><topic>Energy. Thermal use of fuels</topic><topic>Exact sciences and technology</topic><topic>Fission nuclear power plants</topic><topic>Fuels</topic><topic>Installations for energy generation and conversion: thermal and electrical energy</topic><topic>Nuclear fuels</topic><topic>Preparation and processing of nuclear fuels</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hu, Jianwei</creatorcontrib><creatorcontrib>Hayes, A.C.</creatorcontrib><creatorcontrib>Wilson, W.B.</creatorcontrib><creatorcontrib>Rizwan-uddin</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Environmental Engineering Abstracts</collection><collection>Mechanical &amp; Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Nuclear engineering and design</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hu, Jianwei</au><au>Hayes, A.C.</au><au>Wilson, W.B.</au><au>Rizwan-uddin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fission gas production in reactor fuels including the effects of ternary fission</atitle><jtitle>Nuclear engineering and design</jtitle><date>2010-11-01</date><risdate>2010</risdate><volume>240</volume><issue>11</issue><spage>3751</spage><epage>3757</epage><pages>3751-3757</pages><issn>0029-5493</issn><eissn>1872-759X</eissn><coden>NEDEAU</coden><abstract>▶ Noble gas productions were simulated in three different nuclear fuels. ▶ Ternary fission was added into CINDER’90 to track ternary fissioned helium. ▶ Xe has by far the largest production, 136Xe decreases with higher fuel enrichment. ▶ Pu based fuel produces less Kr than U based fuel. ▶ Helium produced mainly from transuranic isotopes. An understanding of gas bubble formation and migration in nuclear fuel and its impacts on fuel and cladding materials requires knowledge of the isotopic composition of the gases and their generation rates. In this paper, we present results of simulations for the production of the dominant noble gases (helium, xenon, krypton) in nuclear fuels for different reactor core configurations and fuel compositions. The calculations were performed using detailed nuclear burn simulations with Monte Carlo nuclear transport, and included ternary fission to ensure an accurate treatment of helium production. For all reactor designs and fuels considered xenon was found to be the most dominant gas produced. Variation in the composition of fission gases is quantified for: (1) the burn time, (2) the composition of the fuel, and (3) the neutron energy spectrum. These three factors determine the relative fraction of each gas and its transmutation into or from stable gas by subsequent neutron capture.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.nucengdes.2010.08.020</doi><tpages>7</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0029-5493
ispartof Nuclear engineering and design, 2010-11, Vol.240 (11), p.3751-3757
issn 0029-5493
1872-759X
language eng
recordid cdi_proquest_miscellaneous_849440847
source ScienceDirect Journals (5 years ago - present)
subjects Applied sciences
Controled nuclear fusion plants
Energy
Energy. Thermal use of fuels
Exact sciences and technology
Fission nuclear power plants
Fuels
Installations for energy generation and conversion: thermal and electrical energy
Nuclear fuels
Preparation and processing of nuclear fuels
title Fission gas production in reactor fuels including the effects of ternary fission
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-06T16%3A36%3A20IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Fission%20gas%20production%20in%20reactor%20fuels%20including%20the%20effects%20of%20ternary%20fission&rft.jtitle=Nuclear%20engineering%20and%20design&rft.au=Hu,%20Jianwei&rft.date=2010-11-01&rft.volume=240&rft.issue=11&rft.spage=3751&rft.epage=3757&rft.pages=3751-3757&rft.issn=0029-5493&rft.eissn=1872-759X&rft.coden=NEDEAU&rft_id=info:doi/10.1016/j.nucengdes.2010.08.020&rft_dat=%3Cproquest_cross%3E849440847%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=849440847&rft_id=info:pmid/&rft_els_id=S0029549310005364&rfr_iscdi=true