Neutronic performance of CANDU reactor fuelling with ThC2/233UC2
233U isotope is used as a booster fissile fuel material in the form of mixed ThC2/233UC2 fuel in a Canada Deuterium Uranium (CANDU) fuel bundle in order to assure the initial criticality at startup. Three different fuel compositions have been used: (1) 97% ThC2+3% 233UC2, (2) 98% ThC2+2% 233UC2 and...
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Veröffentlicht in: | International journal of energy research 2011-02, Vol.35 (2), p.103-111 |
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description | 233U isotope is used as a booster fissile fuel material in the form of mixed ThC2/233UC2 fuel in a Canada Deuterium Uranium (CANDU) fuel bundle in order to assure the initial criticality at startup. Three different fuel compositions have been used: (1) 97% ThC2+3% 233UC2, (2) 98% ThC2+2% 233UC2 and (3) 99% ThC2+1% 233UC2. The temporal variation of the criticality k∞ and the burn‐up values of the reactor have been calculated by full‐power operation for a period of 20 years. The criticality starts by k∞=1.541, 1.355 and 0.995 for modes of (1), (2) and (3) fuel compositions, respectively. A sharp decrease in the criticality has been observed in the first 2 years as a consequence of rapid 233U burnout fuelling with (1) and (2) modes. The criticality becomes quasi‐constant after the second year and remains above k∞∼1.06 for 20 years. After the second year, the CANDU reactor begins to operate practically as a thorium burner. Very high burnup could be achieved with the same fuel materials (up to 500 000 MWday t−1), provided that the fuel rod claddings would be replaced periodically (after every 500 00 or 100 000 MWday t−1). The reactor criticality will be sufficient for fuelling with (1) and (2) modes until a great fraction of the thorium fuel is burnt up. This would reduce fuel fabrication costs and nuclear waste mass for final disposal per unit energy drastically. Copyright © 2010 John Wiley & Sons, Ltd. |
doi_str_mv | 10.1002/er.1760 |
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Three different fuel compositions have been used: (1) 97% ThC2+3% 233UC2, (2) 98% ThC2+2% 233UC2 and (3) 99% ThC2+1% 233UC2. The temporal variation of the criticality k∞ and the burn‐up values of the reactor have been calculated by full‐power operation for a period of 20 years. The criticality starts by k∞=1.541, 1.355 and 0.995 for modes of (1), (2) and (3) fuel compositions, respectively. A sharp decrease in the criticality has been observed in the first 2 years as a consequence of rapid 233U burnout fuelling with (1) and (2) modes. The criticality becomes quasi‐constant after the second year and remains above k∞∼1.06 for 20 years. After the second year, the CANDU reactor begins to operate practically as a thorium burner. Very high burnup could be achieved with the same fuel materials (up to 500 000 MWday t−1), provided that the fuel rod claddings would be replaced periodically (after every 500 00 or 100 000 MWday t−1). The reactor criticality will be sufficient for fuelling with (1) and (2) modes until a great fraction of the thorium fuel is burnt up. This would reduce fuel fabrication costs and nuclear waste mass for final disposal per unit energy drastically. 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J. Energy Res</addtitle><description>233U isotope is used as a booster fissile fuel material in the form of mixed ThC2/233UC2 fuel in a Canada Deuterium Uranium (CANDU) fuel bundle in order to assure the initial criticality at startup. Three different fuel compositions have been used: (1) 97% ThC2+3% 233UC2, (2) 98% ThC2+2% 233UC2 and (3) 99% ThC2+1% 233UC2. The temporal variation of the criticality k∞ and the burn‐up values of the reactor have been calculated by full‐power operation for a period of 20 years. The criticality starts by k∞=1.541, 1.355 and 0.995 for modes of (1), (2) and (3) fuel compositions, respectively. A sharp decrease in the criticality has been observed in the first 2 years as a consequence of rapid 233U burnout fuelling with (1) and (2) modes. The criticality becomes quasi‐constant after the second year and remains above k∞∼1.06 for 20 years. After the second year, the CANDU reactor begins to operate practically as a thorium burner. Very high burnup could be achieved with the same fuel materials (up to 500 000 MWday t−1), provided that the fuel rod claddings would be replaced periodically (after every 500 00 or 100 000 MWday t−1). The reactor criticality will be sufficient for fuelling with (1) and (2) modes until a great fraction of the thorium fuel is burnt up. This would reduce fuel fabrication costs and nuclear waste mass for final disposal per unit energy drastically. Copyright © 2010 John Wiley & Sons, Ltd.</description><subject>burnup</subject><subject>CANDU</subject><subject>criticality</subject><subject>Fuel consumption</subject><subject>Fuelling</subject><subject>Fuels</subject><subject>Nuclear engineering</subject><subject>Nuclear power generation</subject><subject>Nuclear reactor components</subject><subject>Nuclear reactors</subject><subject>thorium</subject><subject>uranium</subject><issn>0363-907X</issn><issn>1099-114X</issn><issn>1099-114X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp90FFPwjAUBeDGaCKi8S_sTRMzuF23lb5JJqIJQWNAeGu67lamg2G7Bfn3jkD0SZ_uw_1ycnIIuaTQoQBBF22H8hiOSIuCED6l4fyYtIDFzBfA56fkzLl3gOZHeYvcjrGubLnKtbdGa0q7VCuNXmm8pD--m3oWla5K65kaiyJfvXmbvFp4k0USdAPGpklwTk6MKhxeHG6bTO8Hk-TBHz0NH5P-yNcBCPAjpqOMm8hgFvVizRE0j1gWqp5BngoIWaZ0mkGmQg4oMopBbFSoME3RUJ6yNrna565t-Vmjq-Qyd7oppVZY1k4KoHFEQ9Fr5PW_knIOjDIR8t9QbUvnLBq5tvlS2a2kIHdrSrRyt2Yjb_Zykxe4_YvJwctB-3uduwq_frSyHzLmjEdyNh7KZzZ5DcRsJhP2DTy7gs4</recordid><startdate>201102</startdate><enddate>201102</enddate><creator>Yıldız, Kadir</creator><creator>Şahi̇n, Necmettin</creator><creator>Alkan, Mahmut</creator><general>John Wiley & Sons, Ltd</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SU</scope><scope>7TB</scope><scope>8FD</scope><scope>C1K</scope><scope>F28</scope><scope>FR3</scope><scope>KR7</scope><scope>L7M</scope><scope>7ST</scope><scope>SOI</scope></search><sort><creationdate>201102</creationdate><title>Neutronic performance of CANDU reactor fuelling with ThC2/233UC2</title><author>Yıldız, Kadir ; Şahi̇n, Necmettin ; Alkan, Mahmut</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2090-53c5d7f5fed586c7e0c753d4a8fe7b9043dacbd0da470e9d1e26fa4aebbef17b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>burnup</topic><topic>CANDU</topic><topic>criticality</topic><topic>Fuel consumption</topic><topic>Fuelling</topic><topic>Fuels</topic><topic>Nuclear engineering</topic><topic>Nuclear power generation</topic><topic>Nuclear reactor components</topic><topic>Nuclear reactors</topic><topic>thorium</topic><topic>uranium</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yıldız, Kadir</creatorcontrib><creatorcontrib>Şahi̇n, Necmettin</creatorcontrib><creatorcontrib>Alkan, Mahmut</creatorcontrib><collection>Istex</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>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><collection>Environment Abstracts</collection><jtitle>International journal of energy research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yıldız, Kadir</au><au>Şahi̇n, Necmettin</au><au>Alkan, Mahmut</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Neutronic performance of CANDU reactor fuelling with ThC2/233UC2</atitle><jtitle>International journal of energy research</jtitle><addtitle>Int. J. Energy Res</addtitle><date>2011-02</date><risdate>2011</risdate><volume>35</volume><issue>2</issue><spage>103</spage><epage>111</epage><pages>103-111</pages><issn>0363-907X</issn><issn>1099-114X</issn><eissn>1099-114X</eissn><abstract>233U isotope is used as a booster fissile fuel material in the form of mixed ThC2/233UC2 fuel in a Canada Deuterium Uranium (CANDU) fuel bundle in order to assure the initial criticality at startup. Three different fuel compositions have been used: (1) 97% ThC2+3% 233UC2, (2) 98% ThC2+2% 233UC2 and (3) 99% ThC2+1% 233UC2. The temporal variation of the criticality k∞ and the burn‐up values of the reactor have been calculated by full‐power operation for a period of 20 years. The criticality starts by k∞=1.541, 1.355 and 0.995 for modes of (1), (2) and (3) fuel compositions, respectively. A sharp decrease in the criticality has been observed in the first 2 years as a consequence of rapid 233U burnout fuelling with (1) and (2) modes. The criticality becomes quasi‐constant after the second year and remains above k∞∼1.06 for 20 years. After the second year, the CANDU reactor begins to operate practically as a thorium burner. Very high burnup could be achieved with the same fuel materials (up to 500 000 MWday t−1), provided that the fuel rod claddings would be replaced periodically (after every 500 00 or 100 000 MWday t−1). The reactor criticality will be sufficient for fuelling with (1) and (2) modes until a great fraction of the thorium fuel is burnt up. This would reduce fuel fabrication costs and nuclear waste mass for final disposal per unit energy drastically. Copyright © 2010 John Wiley & Sons, Ltd.</abstract><cop>Chichester, UK</cop><pub>John Wiley & Sons, Ltd</pub><doi>10.1002/er.1760</doi><tpages>9</tpages></addata></record> |
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subjects | burnup CANDU criticality Fuel consumption Fuelling Fuels Nuclear engineering Nuclear power generation Nuclear reactor components Nuclear reactors thorium uranium |
title | Neutronic performance of CANDU reactor fuelling with ThC2/233UC2 |
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