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Resonance Absorption of Neutrons by Uranium Cylinders
The integrated effective resonance neutron absorption cross section of uranium-238 cylinders has been experimentally investigated in the Hanford Test Pile. The results of reactivity measurements were interpreted to yield the effective resonance integral as a function of the surface-to-mass ratio of...
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Published in: | Journal of applied physics 1957-01, Vol.28 (2), p.250-254 |
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container_end_page | 254 |
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container_title | Journal of applied physics |
container_volume | 28 |
creator | Davis, Monte V. |
description | The integrated effective resonance neutron absorption cross section of uranium-238 cylinders has been experimentally investigated in the Hanford Test Pile. The results of reactivity measurements were interpreted to yield the effective resonance integral as a function of the surface-to-mass ratio of the uranium cylinders. The experiments were extended to determine the Doppler coefficients resulting from heating the uranium in a constant neutron spectrum in the reactor. The effective resonance integral, ∫ (σa0)effdE′/E′, can be approximated as a function of the surface-to-mass ratio by ∫ (σa0)effdE′E′=6.0{1+15.6SM[1−2.18SM+2.19(SM)2]}. The Doppler coefficient of resonance escape probability for the reactor is 1p∂p∂T=(−2.14±0.16)10−5/∘C,and the value assigned to the coefficient of the volume absorption of the resonance integral is 1A∂A∂T=(1.56±0.12)10−4/∘C. |
doi_str_mv | 10.1063/1.1722717 |
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The results of reactivity measurements were interpreted to yield the effective resonance integral as a function of the surface-to-mass ratio of the uranium cylinders. The experiments were extended to determine the Doppler coefficients resulting from heating the uranium in a constant neutron spectrum in the reactor. The effective resonance integral, ∫ (σa0)effdE′/E′, can be approximated as a function of the surface-to-mass ratio by ∫ (σa0)effdE′E′=6.0{1+15.6SM[1−2.18SM+2.19(SM)2]}. The Doppler coefficient of resonance escape probability for the reactor is 1p∂p∂T=(−2.14±0.16)10−5/∘C,and the value assigned to the coefficient of the volume absorption of the resonance integral is 1A∂A∂T=(1.56±0.12)10−4/∘C.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.1722717</identifier><language>eng</language><ispartof>Journal of applied physics, 1957-01, Vol.28 (2), p.250-254</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c351t-336e0d9f5bec3b7c66eff23c653476d62d0bb654d370c20cffd035642a6002dc3</citedby><cites>FETCH-LOGICAL-c351t-336e0d9f5bec3b7c66eff23c653476d62d0bb654d370c20cffd035642a6002dc3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Davis, Monte V.</creatorcontrib><title>Resonance Absorption of Neutrons by Uranium Cylinders</title><title>Journal of applied physics</title><description>The integrated effective resonance neutron absorption cross section of uranium-238 cylinders has been experimentally investigated in the Hanford Test Pile. The results of reactivity measurements were interpreted to yield the effective resonance integral as a function of the surface-to-mass ratio of the uranium cylinders. The experiments were extended to determine the Doppler coefficients resulting from heating the uranium in a constant neutron spectrum in the reactor. The effective resonance integral, ∫ (σa0)effdE′/E′, can be approximated as a function of the surface-to-mass ratio by ∫ (σa0)effdE′E′=6.0{1+15.6SM[1−2.18SM+2.19(SM)2]}. The Doppler coefficient of resonance escape probability for the reactor is 1p∂p∂T=(−2.14±0.16)10−5/∘C,and the value assigned to the coefficient of the volume absorption of the resonance integral is 1A∂A∂T=(1.56±0.12)10−4/∘C.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1957</creationdate><recordtype>article</recordtype><recordid>eNotj8tKxDAUQIMoWEcX_kG2Ljrem9sk7XIovmBQEGddmhdUZpIh6Sz69yrO6uwO5zB2j7BGUPSIa9RCaNQXrEJou1pLCZesAhBYt53urtlNKd8AiC11FZOfvqQ4Ruv5xpSUj_OUIk-Bv_vTnFMs3Cx8l8c4nQ68X_ZTdD6XW3YVxn3xd2eu2O756at_rbcfL2_9ZltbkjjXRMqD64I03pLRVikfgiCrJDVaOSUcGKNk40iDFWBDcEBSNWJUv73O0oo9_HttTqVkH4Zjng5jXgaE4e93wOH8Sz9wRkcU</recordid><startdate>19570101</startdate><enddate>19570101</enddate><creator>Davis, Monte V.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19570101</creationdate><title>Resonance Absorption of Neutrons by Uranium Cylinders</title><author>Davis, Monte V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c351t-336e0d9f5bec3b7c66eff23c653476d62d0bb654d370c20cffd035642a6002dc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1957</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Davis, Monte V.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Davis, Monte V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Resonance Absorption of Neutrons by Uranium Cylinders</atitle><jtitle>Journal of applied physics</jtitle><date>1957-01-01</date><risdate>1957</risdate><volume>28</volume><issue>2</issue><spage>250</spage><epage>254</epage><pages>250-254</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>The integrated effective resonance neutron absorption cross section of uranium-238 cylinders has been experimentally investigated in the Hanford Test Pile. The results of reactivity measurements were interpreted to yield the effective resonance integral as a function of the surface-to-mass ratio of the uranium cylinders. The experiments were extended to determine the Doppler coefficients resulting from heating the uranium in a constant neutron spectrum in the reactor. The effective resonance integral, ∫ (σa0)effdE′/E′, can be approximated as a function of the surface-to-mass ratio by ∫ (σa0)effdE′E′=6.0{1+15.6SM[1−2.18SM+2.19(SM)2]}. The Doppler coefficient of resonance escape probability for the reactor is 1p∂p∂T=(−2.14±0.16)10−5/∘C,and the value assigned to the coefficient of the volume absorption of the resonance integral is 1A∂A∂T=(1.56±0.12)10−4/∘C.</abstract><doi>10.1063/1.1722717</doi><tpages>5</tpages></addata></record> |
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title | Resonance Absorption of Neutrons by Uranium Cylinders |
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