Abstract

For validating the current evaluated neutron data libraries, neutron leakage spectra from lead and lead bismuth eutectic (LBE) cylinders have been measured using an intense D-T pulsed neutron source with time-of-flight (TOF) method by Institute of Nuclear Energy Safety Technology (INEST), Chinese Academy of Sciences (CAS). The measured leakage spectra have been compared with the calculated ones using Super Monte Carlo Simulation Program for Nuclear and Radiation Process (SuperMC) with the evaluated pointwise data of lead and bismuth processed from ENDF/B-VII.1, JEFF-3.1 and JENDL-4.0 libraries. This work shows that calculations of the three libraries are all generally consistent with the lead experimental result. For LBE experiment, the JEFF-3.1 and JENDL-4.0 calculations both agree well with the measurement. However, the result of ENDF/B-VII.1 fails to fit with the measured data, especially in the energy range of 5.5 and 7 MeV with difference more than 80%. Through sensitivity analysis with partial cross sections of 209 Bi in ENDF/B-VII.1 and JEFF, the difference between the measurement and the ENDF/B-VII.1 calculation in LBE experiment is found due to the neutron data of 209 Bi.

Highlights

  • LQFOXGHG WKH VDPSOH LQ DQG VDPSOH RXW PHDVXUHPHQWV 7KH VDPSOH LQ PHDVXUHPHQW DQG VDPSOH RXW VXUYH\ REWDLQHG WKH IRUHJURXQG DQG EDFNJURXQG GDWD UHVSHFWLYHO\ 7KH QHW 72) VSHFWUD ZHUH DFKLHYHG E\ VXEWUDFWLQJ WKH EDFNJURXQG GDWD IURP WKH IRUHJURXQG GDWD 7KH XQFHUWDLQWLHV RI WKH H[SHULPHQWDO GDWD FRQWDLQ WKH VWDWLVWLFDO XQFHUWDLQW\ WKH QHXWURQ GHWHFWLRQ HIILFLHQF\ ̱ DQG WKH QHXWURQ VRXUFH \LHOG.

  • $V VKRZQ LQ )LJXUH DQG 7DEOH IRU 3E VDPSOH LQ WKH HQHUJ\ UDQJH RI 0H9 GLVFUHSDQFLHV EHWZHHQ FDOFXODWLRQV RI WKUHH OLEUDULHV DQG H[SHULPHQW H[FHHG QR PRUH WKDQ ,Q 0H9 UHJLRQ WKH UHVXOW RI -(1'/ XQGHUHVWLPDWHV QHDUO\ ZKLOH WKH &( YDOXHV RI -()) DQG (1')%9,, DUH DQG UHVSHFWLYHO\ 7KH GLIIHUHQFH EHWZHHQ WKH SDUWLDO VSHFWUXP FDOFXODWHG ZLWK -(1'/ DQG REWDLQHG IURP H[SHULPHQW GRHVQ¶W H[FHHG LQ WKH HQHUJ\ UDQJH EHWZHHQ DQG 0H9 DQG FDOFXODWHG UHVXOWV IURP -()) DQG (1')% 9,, LQ WKH VDPH HQHUJ\ UDQJH RYHUHVWLPDWH WKDW IURP PHDVXUHPHQW DQG UHVSHFWLYHO\ :KHQ QHXWURQ HQHUJ\ LV OHVV WKDQ 0H9 DOO RI WKUHH FDOFXODWLRQV H[FHHG WKH PHDVXUHPHQW OHVV WKDQ ,Q JHQHUDO FDOFXODWHG UHVXOWV REWDLQHG IURP (1')%9,, -()) DQG -(1'/ DJUHH ZHOO ZLWK H[SHULPHQWDO UHVXOW DQG WKH FRQFOXVLRQ FRQVLVWV ZLWK &KLNDUD .RQQR¶V HYDOXDWLRQ RQ -(1'/ ZKLOH VPDOO GLVFUHSDQFLHV H[LVWHG LQ SDUWLDO HQHUJ\ LQWHUYDO

  •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

Read more

Summary

Introduction

LQFOXGHG WKH VDPSOH LQ DQG VDPSOH RXW PHDVXUHPHQWV 7KH VDPSOH LQ PHDVXUHPHQW DQG VDPSOH RXW VXUYH\ REWDLQHG WKH IRUHJURXQG DQG EDFNJURXQG GDWD UHVSHFWLYHO\ 7KH QHW 72) VSHFWUD ZHUH DFKLHYHG E\ VXEWUDFWLQJ WKH EDFNJURXQG GDWD IURP WKH IRUHJURXQG GDWD 7KH XQFHUWDLQWLHV RI WKH H[SHULPHQWDO GDWD FRQWDLQ WKH VWDWLVWLFDO XQFHUWDLQW\ WKH QHXWURQ GHWHFWLRQ HIILFLHQF\ ̱ DQG WKH QHXWURQ VRXUFH \LHOG.

Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call