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...
Gespeichert in:
Veröffentlicht in: | Nuclear engineering and design 2010-11, Vol.240 (11), p.3751-3757 |
---|---|
Hauptverfasser: | , , , |
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>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=23403932$$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 & Communications Abstracts</collection><collection>Environmental Engineering Abstracts</collection><collection>Mechanical & 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 |