High Power Laser and Particle Beams, Volume. 36, Issue 6, 066001(2024)

Application of MORPHY program in lead-cooled fast reactor

Jinzhou Li, Tengfei Zhang, Donghao He*, Qingquan Pan, and Xiaojing Liu
Author Affiliations
  • School of Nuclear Science and Engineering, Shanghai Jiao Tong University, Shanghai 200240, China
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    Figures & Tables(24)
    ELSY assembly arrangement
    Different types of grid division
    2D full reactor model
    Single assembly model of different kinds of assemblies
    Normalized flux distribution of 2D model
    Normalized flux deviations distribution of 2D model
    3D model with all control rods (CRs) removed
    Normalized flux deviations distribution of all CRs removed model
    3D model with CRs inserted halfway
    Normalized flux distribution of different insertion modes
    Normalized flux deviation distribution of four inserted-halfway models
    CR fully-inserted model
    Normalized flux distribution of different full insertion modes
    The normalized flux deviation distribution of different full insertion modes
    • Table 1. Material parameters of various fuel assemblies

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      Table 1. Material parameters of various fuel assemblies

      fuel typemass density/(g·cm−3)enrichment /%mass fraction of Pu-U/%
      235U239Pu
      inner fuel11.00490.403856.8714.6
      middle fuel11.00920.403956.8715.5
      outer fuel11.02360.403756.8718.5
    • Table 2. The keff calculation results of different correction methods were added

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      Table 2. The keff calculation results of different correction methods were added

      methodkeff (MORPHY)keff (Serpent)deviation/10−5
      no correction1.025031.00790$ \pm $0.00009+1713
      transport correction1.003921.00790$ \pm $0.00009−398
      (n,xn) correction1.006561.00790$ \pm $0.00009−134
    • Table 3. The keff calculation results of different SN expansion orders

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      Table 3. The keff calculation results of different SN expansion orders

      Model$ {S}_{N} $keffkeff deviation/$ {10}^{-5} $MORPHYcalculation time/(CPU·h)
      MORPHYSerpent
      $ {S}_{2} $1.006561.00790$ \pm $0.00009−1345
      Serpent(2D)$ {S}_{4} $1.007971.00790$ \pm $0.00009+712
      $ {S}_{6} $1.008131.00790$ \pm $0.00009+2327
      $ {S}_{2} $1.004761.00790$ \pm $0.00009−3145
      Serpent(S)$ {S}_{4} $1.005311.00790$ \pm $0.00009−25912
      $ {S}_{6} $1.005281.00790$ \pm $0.00009−26227
    • Table 4. The keff calculation results of 3D model with all CRs removed

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      Table 4. The keff calculation results of 3D model with all CRs removed

      modelkeff calculation resultsdeviation/10−5
      keff (MORPHY)keff (Serpent)
      all CRs removed0.995720.99594$ \pm $0.00008−22
    • Table 5. The keff calculation results of 3D full reactor model with CRs inserted halfway

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      Table 5. The keff calculation results of 3D full reactor model with CRs inserted halfway

      modelkeff calculation resultsdeviation/10−5
      MORPHYSerpent
      all CRs inserted halfway0.976910.97729$ \pm $0.00008−38
      only CR A inserted halfway0.995070.99486$ \pm $0.00007+21
      only CR C inserted halfway0.995160.99514$ \pm $0.00007+2
      CRs A and B inserted halfway0.994380.99454$ \pm $0.00007−16
    • Table 6. The calculation results of reactivity change of 3D full reactor with CRs inserted halfway

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      Table 6. The calculation results of reactivity change of 3D full reactor with CRs inserted halfway

      modelreactivity of MORPHYreactivity of Serpentdeviation/10−5
      all CRs insert halfway18811865+16
      only CR A insert halfway65108−43
      only CR C insert halfway5680−24
      CRs A and B insert halfway134140−6
    • Table 7. Flux deviation of 3D full reactor with CRs inserted halfway

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      Table 7. Flux deviation of 3D full reactor with CRs inserted halfway

      modelmin negative deviation/%max positive deviation/%mean absolute deviation/%
      only A inserted halfway−6.572.971.60
      only C inserted halfway−8.873.191.70
      CRs A and B inserted halfway−9.733.111.76
    • Table 8. The keff calculation results of three dimensional full reactor model with CRs fully inserted

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      Table 8. The keff calculation results of three dimensional full reactor model with CRs fully inserted

      modelkeff calculation results
      MORPHYSerpentdeviation/10−5
      all CRs fully insert0.969110.96888$ \pm $0.00008+23
      only CR A fully insert0.994310.99460$ \pm $0.00007−29
      only CR C fully insert0.994400.99470$ \pm $0.00007−30
      CR A and B fully insert0.994050.99429$ \pm $0.00007−24
    • Table 9. The calculation results of CR worth for CR assembly

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      Table 9. The calculation results of CR worth for CR assembly

      modelCR worth calculation results
      MORPHY/10−5Serpent/10−5deviation/10−5
      all CRs fully insert26612706−45
      only CR A fully insert141134+7
      only CR C fully insert132124+8
      CR A and B fully insert167165+2
    • Table 10. The flux calculation deviation of 3D full reactor with CRs fully inserted

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      Table 10. The flux calculation deviation of 3D full reactor with CRs fully inserted

      modelmin negative deviation/%max positive deviation/%mean absolute deviation/%
      all CRs fully inserted−7.681.621.81
      only CR A fully inserted−5.392.841.62
      only CR C fully inserted−5.683.431.78
      CR A and B fully inserted−5.852.111.37
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    Jinzhou Li, Tengfei Zhang, Donghao He, Qingquan Pan, Xiaojing Liu. Application of MORPHY program in lead-cooled fast reactor[J]. High Power Laser and Particle Beams, 2024, 36(6): 066001

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    Paper Information

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    Received: Oct. 17, 2023

    Accepted: Jan. 31, 2024

    Published Online: Jun. 3, 2024

    The Author Email: Donghao He (donghaohe@sjtu.edu.cn)

    DOI:10.11884/HPLPB202436.230357

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