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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Energy Res.</journal-id>
<journal-title>Frontiers in Energy Research</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Energy Res.</abbrev-journal-title>
<issn pub-type="epub">2296-598X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">764905</article-id>
<article-id pub-id-type="doi">10.3389/fenrg.2021.764905</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Energy Research</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Physical Design of High-Performance Fuel Assembly Based on Fully Ceramic Microencapsulated Fuel for Supercritical CO<sub>2</sub> Cooled Reactor</article-title>
<alt-title alt-title-type="left-running-head">Lu et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Supercritical CO<sub>2</sub> Cooled Reactor</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Lu</surname>
<given-names>Di</given-names>
</name>
<uri xlink:href="https://loop.frontiersin.org/people/1456034/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wang</surname>
<given-names>Lianjie</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1340943/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Cai</surname>
<given-names>Yun</given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wang</surname>
<given-names>Dongyong</given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhang</surname>
<given-names>Ce</given-names>
</name>
</contrib>
</contrib-group>
<aff>Nuclear Power Institute of China (NPIC), <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/447098/overview">Jun Wang</ext-link>, University of Wisconsin-Madison, United&#x20;States</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/493311/overview">Jie Cheng</ext-link>, Harbin Engineering University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1076661/overview">Guang Hu</ext-link>, Xi&#x2019;an Jiaotong University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Lianjie Wang, <email>mcd2264@126.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Nuclear Energy, a section of the journal Frontiers in Energy Research</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>25</day>
<month>11</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>9</volume>
<elocation-id>764905</elocation-id>
<history>
<date date-type="received">
<day>26</day>
<month>08</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>25</day>
<month>10</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Lu, Wang, Cai, Wang and Zhang.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Lu, Wang, Cai, Wang and Zhang</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Fully ceramic microencapsulated fuel (FCM) is employed in the supercritical CO<sub>2</sub> (S-CO<sub>2</sub>)-cooled reactor as accident tolerant fuel (ATF). Although the fuel and the assembly substrate contain SiC, the assembly cannot be sufficiently moderated due to the weak moderating performance of S-CO<sub>2</sub>, which affects the neutronics economy seriously. In this study, a new fuel assembly based on FCM fuel is proposed for the S-CO<sub>2</sub> cooled reactor. Besides, the solid moderator rod is introduced into the design. Although the introduction of moderator rods can effectively improve the moderation performance of S-CO<sub>2</sub> reactor assembly, it will lead to the deterioration of uniform moderation. To further improve the uniform moderation, arrangement of moderator rods and fuel enrichment partition are studied. Finally, the results show clearly that a better balance between uniform moderation and sufficient moderation can be obtained in the high-performance S-CO<sub>2</sub> reactor assembly.</p>
</abstract>
<kwd-group>
<kwd>supercritical CO<sub>2</sub> cooled reactor</kwd>
<kwd>fuel assembly (FA)</kwd>
<kwd>FCM fuel</kwd>
<kwd>sufficient moderation</kwd>
<kwd>uniform moderation</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>By taking advantage of the appropriate critical pressure, high density, stability, and sluggishness of CO<sub>2</sub> near its critical point, the use of supercritical CO<sub>2</sub>(S-CO<sub>2</sub>) as a coolant in the direct cycle reactor is evaluated (<xref ref-type="bibr" rid="B1">Ahn et&#x20;al., 2015</xref>; <xref ref-type="bibr" rid="B6">Wu et&#x20;al., 2020</xref>). The S-CO<sub>2</sub>&#x2013;cooled reactor, as a promising innovative reactor, has the advantages of simple system, high thermal efficiency, small volume, and light weight, and it represents an important development direction for nuclear energy innovation and development (<xref ref-type="bibr" rid="B4">Michael, 2004</xref>).</p>
<p>Safety and economics are the main objectives of the S-CO<sub>2</sub>&#x2013;cooled reactor. A new fuel concept is referred to as accident-tolerant fuels (ATFs) are capable of mitigating the potential consequences of beyond-design-basis accidents (<xref ref-type="bibr" rid="B3">Bragg-Sitton, 2014</xref>). The fully ceramic microencapsulated (FCM) fuel (<xref ref-type="bibr" rid="B5">Terrani et&#x20;al., 2012</xref>) has become one among the ATF options which is based on tristructural isotropic (TRISO) (<xref ref-type="bibr" rid="B2">Bragg-Sitton and Carmack, 2015</xref>)&#x2013;coated particles embedded in&#x20;silicon carbide (SiC) matrix. FCM fuel borrows from the TRISO particle design from the high-temperature gas reactor (HTGR) technology but uses SiC as a matrix material rather than graphite in HTGR. Benefiting from the multiple barriers of TRISO and SiC matrix, FCM fuel has extremely high radioactivity retention capability compared to that of the conventional standard UO<sub>2</sub> fuel. By the advantages of safety, a new fuel assembly based on the FCM fuel is proposed for the S-CO<sub>2</sub>&#x2013;cooled reactor in this&#x20;study.</p>
<p>In further research, although the FCM fuel contains moderation materials such as SiC, the assembly cannot be sufficiently moderated due to the weak moderating performance of S-CO<sub>2</sub>, which affects the neutronics economy seriously. The study on improving the deficiency of weak moderating performance is described in this article.</p>
<p>Unlike the light water moderated or heavy water moderated (<xref ref-type="bibr" rid="B7">Zhang et al.,2019</xref>; <xref ref-type="bibr" rid="B8">Zhang et al.,2020</xref>) nuclear reactors, the S-CO<sub>2</sub> cooled reactor needs specific moderator rods to improve the slow-down of neutrons. The introduction of moderator rods can effectively improve the moderating performance of S-CO<sub>2</sub>&#x2013;cooled reactor, but it will lead to the deterioration of uniform moderation. To further improve the uniform moderation, moderator rod arrangement and fuel enrichment partition method are studied. Finally, this study shows clearly that a better balance between uniform moderation and sufficient moderation can be&#x20;obtained in the high-performance S-CO<sub>2</sub>&#x2013;cooled reactor assembly.</p>
</sec>
<sec id="s2">
<title>Fully Ceramic Microencapsulated Fuel Assembly of S-CO<sub>2</sub>&#x2013;Cooled Reactor Design</title>
<sec id="s2-1">
<title>Standard Fuel Assembly of S-CO<sub>2</sub>&#x2013;Cooled Reactor Design</title>
<p>An FCM fuel with a TRISO particle is shown in <xref ref-type="fig" rid="F1">Figure&#x20;1</xref>. The TRISO particle geometry and composition are given in <xref ref-type="table" rid="T1">Table&#x20;1</xref> and the FCM fuel design parameters are given in <xref ref-type="table" rid="T2">Table&#x20;2</xref>. In this design, the TRISO particles account for 40% of the volume in FCM fuel and the enrichment of <sup>235</sup>U reaches 19.75%.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Design of FCM&#x20;fuel.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g001.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>TRISO particle geometry and composition.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Layer</th>
<th align="center">Radius (mm)</th>
<th align="center">Density (g/cm<sup>3</sup>)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Kernel</td>
<td align="char" char=".">0.4000</td>
<td align="char" char=".">10.41</td>
</tr>
<tr>
<td align="left">Porous carbon buffer</td>
<td align="char" char=".">0.4500</td>
<td align="char" char=".">1.100</td>
</tr>
<tr>
<td align="left">Inner pyrolytic carbon</td>
<td align="char" char=".">0.4850</td>
<td align="char" char=".">1.900</td>
</tr>
<tr>
<td align="left">Silicon carbide</td>
<td align="char" char=".">0.5200</td>
<td align="char" char=".">3.180</td>
</tr>
<tr>
<td align="left">Outer pyrolytic carbon</td>
<td align="char" char=".">0.5400</td>
<td align="char" char=".">1.900</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>FCM fuel design parameters.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Parameter</th>
<th align="center">Value</th>
<th align="center">Unit</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Fuel compact outer radius</td>
<td align="char" char=".">8.3500</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">Gas gap outer radius</td>
<td align="char" char=".">8.4000</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">SiC Clad outer radius</td>
<td align="char" char=".">8.9000</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">
<sup>235</sup>U enrichment</td>
<td align="char" char=".">19.75%</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">TRISO particle share</td>
<td align="char" char=".">40%</td>
<td align="center">-</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The standard fuel assembly of S-CO<sub>2</sub>&#x2013;cooled reactor in this study is shown in <xref ref-type="fig" rid="F2">Figure&#x20;2</xref>; it contains SiC block, fuel holes, coolant holes, and lumped burnable poison (or control rods) hole. The assembly design parameters are given in <xref ref-type="table" rid="T3">Table&#x20;3</xref>. Each block is a right hexagonal prism with a dimension of 2,500&#xa0;mm in length and 240&#xa0;mm across the flats of the hexagonal cross section. Fuel and coolant holes run parallel through the length of the block in a regular triangular pattern of nominally two fuel holes per coolant hole. The pitch of the fuel and coolant hole array is 18&#xa0;mm. The minimum web thickness between the fuel hold and coolant hole is 6&#xa0;mm and this web provides an additional barrier to the release of metallic fission products. In order to get an effective control of reactivity, a lumped burnable poison (or control rods) hole (72&#xa0;mm) is added to the center of standard fuel assembly.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>S-CO<sub>2</sub>&#x2013;cooled reactor standard fuel assembly.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g002.tif"/>
</fig>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>FCM fuel design parameters.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Parameter</th>
<th align="center">Value</th>
<th align="center">Unit</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">SiC block length</td>
<td align="char" char=".">2,500.00</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">SiC block width</td>
<td align="char" char=".">240.00</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">Fuel/Coolant hold diameter</td>
<td align="char" char=".">18.00</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">Minimum web thickness</td>
<td align="char" char=".">6.00</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">SiC Clad outer radius</td>
<td align="char" char=".">8.90</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">lumped burnable poison (or control rods) hole diameter</td>
<td align="char" char=".">72.00</td>
<td align="center">mm</td>
</tr>
<tr>
<td align="left">Fuel hold number</td>
<td align="char" char=".">54</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Coolant hold number</td>
<td align="char" char=".">30</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">U weight per assembly</td>
<td align="char" char=".">44.48</td>
<td align="center">kg</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-2">
<title>Neutron Moderating Performance Analysis for the Standard Assembly</title>
<p>To analyze neutron moderating performance for the standard assembly, the light water (H<sub>2</sub>O) coolant fuel assembly is used for comparison in standard assembly cooling by S-CO<sub>2</sub>. Other than replacing coolant with H<sub>2</sub>O, the design parameters remain unchanged to compare S-CO<sub>2</sub> assembly and H<sub>2</sub>O assembly in moderating analyses. The calculation in the study is done by using HANDF-E code package developed by the Nuclear Power Institute of China. This code has been used in the analysis of hexagonal assembly because of its high accuracy.</p>
<p>Infinite multiplication factor (<inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>) is the main parameter that characterizes fuel reactivity. In general, moderating performance largely determines the value of <inline-formula id="inf2">
<mml:math id="m2">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. <inline-formula id="inf3">
<mml:math id="m3">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>of each assembles as fuel burn up varies, as shown in <xref ref-type="fig" rid="F3">Figure&#x20;3</xref>. <inline-formula id="inf4">
<mml:math id="m4">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>of&#x20;S-CO<sub>2</sub> assembly is much less than that of H<sub>2</sub>O under the same fuel burn up. The calculation results clearly show that S-CO<sub>2</sub> assembly has the defect of insufficient moderating performance.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>
<inline-formula id="inf5">
<mml:math id="m5">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> versus fuel burn&#x20;up.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g003.tif"/>
</fig>
<p>Neutrons can be moderated in the SiC, and increasing the SiC matrix share of FCM fuel is the most direct way to improve the moderating performance. The SiC matrix share increases from 60 to 80%, or even 90%, and then <inline-formula id="inf6">
<mml:math id="m6">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> by different SiC matrix share as fuel burn up varies is shown in <xref ref-type="fig" rid="F4">Figure&#x20;4</xref>. The calculation results clearly show that increasing SiC matrix share is beneficial to enhance moderating performance and improve fuel reactivity. <xref ref-type="fig" rid="F4">Figure&#x20;4</xref> also presents <inline-formula id="inf7">
<mml:math id="m7">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> of H<sub>2</sub>O assembly by different SiC matrix share as fuel burn up varies. Even if the matrix share changes, <inline-formula id="inf8">
<mml:math id="m8">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> of H<sub>2</sub>O is still much greater than that of S-CO<sub>2</sub>. These results show that the method of increasing the SiC matrix share has a limited effect on improving the moderating performance.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>
<inline-formula id="inf9">
<mml:math id="m9">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> by different SiC matrix share versus burn&#x20;up.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g004.tif"/>
</fig>
<p>In fact, in terms of fuel burn up and core volume, increasing SiC matrix share is not a good idea; it means the TRISO particle share is reduced and fuel burn up will be grow greatly. To reduce fuel burn up, a larger number of assembles will be used in core, resulting in a larger core volume, and the large core volume makes the design of pressure vessels under high temperature and pressure a great challenge. Therefore, the method to improve the moderating performance should minimize the increase in core volume.</p>
</sec>
</sec>
<sec id="s3">
<title>Neutronics Analysis for the Design of YH<sub>1.8</sub> in the Standard Assembly</title>
<p>Because of stronger neutron moderating capacity, metal hydride has been used as a solid moderator in reactors. Yttrium hydride (YH<sub>1.8</sub>) is more suitable to use in the S-CO<sub>2</sub> cooled reactor because it is more stable than zirconium hydride (ZrH<sub>1.6</sub>) at high temperature.</p>
<p>The design of YH<sub>1.8</sub> solid moderator rod used in this study is&#x20;shown in <xref ref-type="fig" rid="F5">Figure&#x20;5</xref>. To reduce the release of hydrogen atoms, the solid moderator rod is coated with stainless steel. The YH<sub>1.8</sub> solid moderator rod geometry and composition are given in <xref ref-type="table" rid="T4">Table&#x20;4</xref>.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>YH<sub>1.8</sub> solid moderator&#x20;pin.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g005.tif"/>
</fig>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>YH<sub>1.8</sub> solid moderator pin geometry and composition.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Layer</th>
<th align="center">Radius (mm)</th>
<th align="center">Material</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Kernel</td>
<td align="char" char=".">8.4000</td>
<td align="center">YH<sub>1.8</sub>
</td>
</tr>
<tr>
<td align="left">Cladding</td>
<td align="char" char=".">8.9000</td>
<td align="center">stainless steel</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The moderating method is to insert the YH<sub>1.8</sub> solid moderator rod into part of fuel holds instead of the FCM fuel. The moderating performance of assembly can be changed by using different number of YH<sub>1.8</sub> solid moderator rods. The number of YH<sub>1.8</sub> solid moderator rod analyzed in this study is shown in <xref ref-type="table" rid="T5">Table&#x20;5</xref>, and the arrangements of the YH<sub>1.8</sub> solid moderator rods are shown in <xref ref-type="fig" rid="F6">Figure&#x20;6</xref>.</p>
<table-wrap id="T5" position="float">
<label>TABLE 5</label>
<caption>
<p>YH<sub>1.8</sub> solid moderator rods number setting.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="center">YH<sub>1.8</sub> rods number</th>
<th align="center">Fuel rods number</th>
<th align="center">Relative share of fuel</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">1</td>
<td align="char" char=".">0</td>
<td align="char" char=".">54</td>
<td align="char" char=".">1.000</td>
</tr>
<tr>
<td align="left">2</td>
<td align="char" char=".">6</td>
<td align="char" char=".">48</td>
<td align="char" char=".">0.889</td>
</tr>
<tr>
<td align="left">3</td>
<td align="char" char=".">12</td>
<td align="char" char=".">42</td>
<td align="char" char=".">0.778</td>
</tr>
<tr>
<td align="left">4</td>
<td align="char" char=".">18</td>
<td align="char" char=".">36</td>
<td align="char" char=".">0.667</td>
</tr>
<tr>
<td align="left">5</td>
<td align="char" char=".">24</td>
<td align="char" char=".">30</td>
<td align="char" char=".">0.556</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Arrangements of YH<sub>1.8</sub> solid moderator rods in S-CO<sub>2</sub> assembly.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g006.tif"/>
</fig>
<p>
<inline-formula id="inf10">
<mml:math id="m10">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> by different YH<sub>1.8</sub> solid moderator rod number as fuel burn up varies is shown in <xref ref-type="fig" rid="F7">Figure&#x20;7</xref>. The calculation results clearly show that adding YH<sub>1.8</sub> solid moderator rod can significantly enhance moderating performance and then improve the fuel reactivity greatly. <inline-formula id="inf11">
<mml:math id="m11">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> of H<sub>2</sub>O is also described in <xref ref-type="fig" rid="F6">Figure&#x20;6</xref>. When the number of YH<sub>1.8</sub> solid moderator rods is greater than 12, the <inline-formula id="inf12">
<mml:math id="m12">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>of S-CO<sub>2</sub> assembly is significantly larger than that of H<sub>2</sub>O assembly. These results show that moderating performance can be improved significantly by inserting the YH<sub>1.8</sub> solid moderator rod. When 12 YH<sub>1.8</sub> solid moderator rods were inserted, the S-CO<sub>2</sub> assembly was moderated sufficiently and the fuel share was reduced by only&#x20;22.2%.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>
<inline-formula id="inf13">
<mml:math id="m13">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> by different numbers of YH<sub>1.8</sub> rods versus burn&#x20;up.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g007.tif"/>
</fig>
<p>The moderating effect of different materials was further studied. Commonly used moderating materials such as graphite and BeO are used for comparison with YH<sub>1.8</sub>. <inline-formula id="inf14">
<mml:math id="m14">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> of different moderating materials as fuel burn up varies are shown in <xref ref-type="fig" rid="F8">Figure&#x20;8</xref>. <inline-formula id="inf15">
<mml:math id="m15">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> of YH<sub>1.8</sub> is significantly larger than that of graphite and BeO. The results show that using YH<sub>1.8</sub> as a moderator is the best choice to improve the moderating performance of S-CO<sub>2</sub> assembly.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>
<inline-formula id="inf16">
<mml:math id="m16">
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>&#x221e;</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> by different moderating materials versus burn&#x20;up.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g008.tif"/>
</fig>
</sec>
<sec id="s4">
<title>Uniform Moderating Design for the S-CO<sub>2</sub> Assembly</title>
<p>Inserting the YH<sub>1.8</sub> solid moderator rods cause uneven moderating in the assembly. In order to get uniform moderating, the arrangement of the moderators must be studied.</p>
<p>The moderating effect and the change of fuel share were considered, and then the number of YH<sub>1.8</sub> solid moderator rods is selected as 12 in this section. The different arrangements of YH<sub>1.8</sub> solid moderator rods are shown in <xref ref-type="fig" rid="F9">Figure&#x20;9</xref> and power uneven factor by different solid moderator arrangements as fuel burn up varies are shown in <xref ref-type="fig" rid="F10">Figure&#x20;10</xref>. The arrangement B of solid moderator obtains the lowest uneven factor and becomes the preferred arrangement in this&#x20;study.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>Arrangements of 12 YH<sub>1.8</sub> solid moderator&#x20;rods.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Power uneven factor by different solid moderator arrangements.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g010.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F11">Figure&#x20;11</xref> presents the BOL (<bold>B</bold>egin <bold>O</bold>f <bold>L</bold>ife) relative power distribution of S-CO<sub>2</sub> assembly using arrangement B. <xref ref-type="fig" rid="F11">Figure&#x20;11</xref> clearly shows that the maximum power is at site A and the minimum power is at site B. In order to further realize the uniform moderating to reduce the power uneven factor, the fuel share of FCM partitioning method is applied in the S-CO<sub>2</sub> assembly design. The fuel share of FCM is reduced from 40 to 35% at site A which have maximum power and the fuel share of FCM is increased from 40 to 45% at site B which have minimum power. In addition, this partitioning method ensures that the fuel weight remains the same in the S-CO<sub>2</sub> assembly. The BOL relative power distribution of S-CO<sub>2</sub> assembly using the partitioning method is shown in <xref ref-type="fig" rid="F12">Figure&#x20;12</xref>. The relative power at site A decreases from 1.069 to 0.964, the relative power at site B increases from 0.915 to 1.005, and then the uneven factor decreases from 1.069 to 1.028. <xref ref-type="fig" rid="F13">Figure&#x20;13</xref> presents a power uneven factor by arrangement B with the partitioning method as fuel burn up varies; it shows that the fuel share of the FCM partitioning method can achieve more uniform moderating and power distribution.</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Relative power distribution of S-CO<sub>2</sub> assembly using arrangement B (BOL).</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g011.tif"/>
</fig>
<fig id="F12" position="float">
<label>FIGURE 12</label>
<caption>
<p>Relative power distribution of S-CO<sub>2</sub> assembly using the partitioning method (BOL).</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g012.tif"/>
</fig>
<fig id="F13" position="float">
<label>FIGURE 13</label>
<caption>
<p>Power uneven factor by arrangement B with the partitioning method.</p>
</caption>
<graphic xlink:href="fenrg-09-764905-g013.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s5">
<title>Conclusion</title>
<p>As a new type reactor with development potential, the S-CO<sub>2</sub>&#x2013;cooled reactor has many advantages, such as simple system, high thermal efficiency, and small volume. FCM fuel which is a potential option of ATF is capable to mitigate the&#x20;potential consequences of beyond-design-basis accidents and become the preferred type of fuel for the S-CO<sub>2</sub>&#x2013;cooled reactor.</p>
<p>In this article, a new fuel assembly design concept based on FCM fuel for S-CO<sub>2</sub>&#x2013;cooled reactor is proposed. Then, the design of YH<sub>1.8</sub> solid moderator rod was adopted to improve the moderating performance of the fuel assembly. In order to deal with the moderating non-uniformity caused by the moderator, the arrangement of moderators and the method of fuel share partitioning were well studied, and then the high-performance fuel assembly based on FCM fuel for S-CO<sub>2</sub>&#x2013;cooled reactor is proposed at last. The main conclusions of the study are as follows:<list list-type="simple">
<list-item>
<p>1) The fuel assembly based on the FCM fuel for the S-CO<sub>2</sub>&#x2013;cooled reactor was proposed because of the safety advantage. Due to the weak moderating performance of S-CO<sub>2</sub>, the neutrons in this assembly cannot be sufficiently moderated and affects the neutronics economy seriously.</p>
</list-item>
<list-item>
<p>2) As it is superior to the method of adjusting the SiC matrix&#x20;share, the design of YH<sub>1.8</sub> solid moderator rod is studied. With this design, the assembly can be sufficiently moderated.</p>
</list-item>
<list-item>
<p>3) The arrangement of YH<sub>1.8</sub> solid moderator rods is proposed, which can effectively improve the uniformity of moderating. The method of fuel share partitioning is studied at last and the fuel assembly is further uniformly moderated.</p>
</list-item>
<list-item>
<p>4) The high-performance fuel assembly based on the FCM fuel which has good safety and economics is suitable for S-CO<sub>2</sub>&#x2013;cooled reactor.</p>
</list-item>
</list>
</p>
</sec>
</body>
<back>
<sec id="s6">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s7">
<title>Author Contributions</title>
<p>DL contributed to conceptualization, methodology, and design. LW contributed to conceptualization and methodology. YC performed the calcualtion and analysis. DW funding acquisition and supervision. CZ visualization and investigation.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>This work is supported by the National Natural Science Foundation of China (Approved no.: 12,075,228).</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s10">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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