<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-19T08:04:41Z</responseDate><request verb="GetRecord" identifier="oai:dspace.mit.edu:1721.1/76931" metadataPrefix="dim">https://dspace.mit.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:dspace.mit.edu:1721.1/76931</identifier><datestamp>2022-01-13T07:54:37Z</datestamp><setSpec>com_1721.1_7582</setSpec><setSpec>com_1721.1_7581</setSpec><setSpec>col_1721.1_131024</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="advisor" lang="en_US">Benoit Forget.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Bean, Malcolm (Malcolm K.)</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="other" lang="en_US">Massachusetts Institute of Technology. Dept. of Mathematics.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Mathematics</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Nuclear Science and Engineering</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2013-02-14T15:18:54Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2013-02-14T15:18:54Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2011</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">http://hdl.handle.net/1721.1/76931</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="oclc" lang="en_US">824426933</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Thesis (S.B.)--Massachusetts Institute of Technology, Dept. of Nuclear Science and Engineering; and, (S.B.)--Massachusetts Institute of Technology, Dept. of Mathematics, 2011.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">"May 2011." Cataloged from PDF version of thesis.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Includes bibliographical references (p. 28).</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">Training, Research, Isotopes, General Atomics (TRIGA) reactors have the unique capability of generating high neutron flux environments with the removal of a transient control rod, creating conditions observed in fast fission reactors. Recently, several TRIGA reactors have had issues with the deformation of fuel rods nearest the transient control rod, where the neutron flux is highest. This is a difficult problem to analyze because the damage is not simply due to rods overheating, but rather the pressurization of hydrogen, from the Uranium Hydride fuel, that has diffused into the spacing between fuel and cladding. Previous neutronic analyses utilized point kinetics; a model which assumes changes in reactivity uniformly affect the reactor's flux, resulting in no relative spatial variation over time. Point kinetics is attractive because of its low computing costs, however the pulse's localization, theoretically, should generate a pronounced flux spike and radial neutron wave, which violates an assumption of point kinetics. The aim of the research is not to explicitly describe the cause of fuel rod deformation, but rather generate time dependent, high-resolution 3-dimensional flux maps. The Purdue Advance Reactor Core Simulator (PARCS) was used to simulate a TRIGA pulse with both nodal and point kinetics. Assuming our nodal kinetics models accurately simulate TRIGA pulses, we find that point kinetics methods are ill suited to simulate TRIGA pulses. By maintaining the steady-state flux profile, point kinetics does not capture the fact that the power peak actually occurs in the center assembly, from which the transient control rod is removed. In our simulations, point kinetics underestimated the normalize power in the central assembly by as much as 46.19%.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="statementofresponsibility" lang="en_US">by Malcolm Bean.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="degree" lang="en_US">S.B.</dim:field>
   <dim:field mdschema="dc" element="format" qualifier="extent" lang="en_US">28 p.</dim:field>
   <dim:field mdschema="dc" element="language" qualifier="iso" lang="en_US">eng</dim:field>
   <dim:field mdschema="dc" element="publisher" lang="en_US">Massachusetts Institute of Technology</dim:field>
   <dim:field mdschema="dc" element="rights" lang="en_US">M.I.T. theses are protected by 
copyright. They may be viewed from this source for any purpose, but 
reproduction or distribution in any format is prohibited without written 
permission. See provided URL for inquiries about permission.</dim:field>
   <dim:field mdschema="dc" element="rights" qualifier="uri" lang="en_US">http://dspace.mit.edu/handle/1721.1/7582</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">Nuclear Science and Engineering.</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">Mathematics.</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">Computational neutronics analysis of TRIGA reactors during power pulsing</dim:field>
   <dim:field mdschema="dc" element="title" qualifier="alternative" lang="en_US">Computational neutronics analysis of Training, Research, Isotopes, General Atomics reactors during power pulsing</dim:field>
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   	&lt;Title>Computational neutronics analysis of TRIGA reactors during power pulsing&lt;/Title>
   	&lt;Subtitle>Computational neutronics analysis of Training, Research, Isotopes, General Atomics reactors during power pulsing&lt;/Subtitle>
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   	&lt;PublicationDate>2011&lt;/PublicationDate>
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        	&lt;DisplayName>Bean, Malcolm (Malcolm K.)&lt;/DisplayName>
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            &lt;DisplayName>Massachusetts Institute of Technology&lt;/DisplayName>
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    &lt;Keyword>Nuclear Science and Engineering.&lt;/Keyword>
    &lt;Keyword>Mathematics.&lt;/Keyword>
   	&lt;Abstract>Training, Research, Isotopes, General Atomics (TRIGA) reactors have the unique capability of generating high neutron flux environments with the removal of a transient control rod, creating conditions observed in fast fission reactors. Recently, several TRIGA reactors have had issues with the deformation of fuel rods nearest the transient control rod, where the neutron flux is highest. This is a difficult problem to analyze because the damage is not simply due to rods overheating, but rather the pressurization of hydrogen, from the Uranium Hydride fuel, that has diffused into the spacing between fuel and cladding. Previous neutronic analyses utilized point kinetics; a model which assumes changes in reactivity uniformly affect the reactor&amp;apos;s flux, resulting in no relative spatial variation over time. Point kinetics is attractive because of its low computing costs, however the pulse&amp;apos;s localization, theoretically, should generate a pronounced flux spike and radial neutron wave, which violates an assumption of point kinetics. The aim of the research is not to explicitly describe the cause of fuel rod deformation, but rather generate time dependent, high-resolution 3-dimensional flux maps. The Purdue Advance Reactor Core Simulator (PARCS) was used to simulate a TRIGA pulse with both nodal and point kinetics. Assuming our nodal kinetics models accurately simulate TRIGA pulses, we find that point kinetics methods are ill suited to simulate TRIGA pulses. By maintaining the steady-state flux profile, point kinetics does not capture the fact that the power peak actually occurs in the center assembly, from which the transient control rod is removed. In our simulations, point kinetics underestimated the normalize power in the central assembly by as much as 46.19%.&lt;/Abstract>
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