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    <identifier>10.57760/sciencedb.04925</identifier>
    <datestamp>2022-10-28T11:27:46Z</datestamp>
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  <dc:date>2022-10-28</dc:date>
  <dc:title>Evaluation of tritium burnup fraction for  CFETR scenarios with core-edge coupling  simulations</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.04925</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>A key mission for the next-step fusion tokamak device China Fusion Engineering Test Reactor&amp;nbsp; (CFETR) is demonstrating tritium self-sufficiency, which requires a sufficiently high tritium&amp;nbsp; burnup fraction (fburnup) in order to match a practically achievable tritium breeding ratio&amp;nbsp; (TBR) with the blanket design constraints. Core-edge coupling simulations are performed to&amp;nbsp; investigate the dependence of fburnup on different controlling parameters for CFETR scenarios.&amp;nbsp;Core plasma profiles with a range of pedestal densities are simulated by consistent iterative&amp;nbsp;calculations of equilibrium, transport, auxiliary heating and current drives within the OMFIT&amp;nbsp;framework. The core-SOL integrated COREDIV code is then used to evaluate fburnup with&amp;nbsp;the OMFIT modelled core plasma parameters as input. According to the simulations, fburnup can be effectively increased with a higher pedestal density on account of the fusion power&amp;nbsp; increasing faster than the fueling source required to maintain steady-state. Higher ne,sep/ne,pedcan also increase the fburnup due to increase of fuel recycling. Deeper pellet fueling deposition&amp;nbsp;and lower ratio of particle to thermal diffusivities D/&amp;chi; can both increase the effective particle&amp;nbsp;confinement time and thus fburnup. However, the effect of helium and other impurities (Ar and&amp;nbsp;W) is shown to reduce fburnup for comparable impurity and main ion transport. Based on our&amp;nbsp;analysis, using present pellet fueling technology, achieving fburnup &amp;gt; 3% for CFETR will be&amp;nbsp;very challenging. This is a lower limit for the required TBR (&amp;gt;1) to match the achievable&amp;nbsp;TBR for tritium self-sufficiency. Furthermore, our study suggests that if fueling can penetrate&amp;nbsp;deeper than r/a &amp;lt; 0.8 under optimistic conditions, the required burnup fraction could be&amp;nbsp;attainable. The modelling results thus provide important suggestions and implications for the&amp;nbsp;optimization of CFETR scenarios and development of advanced fueling systems.</dc:description>
  <dc:subject>CFETR; tritium burnup fraction;  core-edge simulations</dc:subject>
  <dc:creator>xie hai</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/https://doi.org/10.1088/1741-4326/ab742b</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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