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    KCI등재 SCIE SCOPUS

    Electron Accelerator Shielding Design of KIPT Neutron Source Facility

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    https://www.riss.kr/link?id=A103658731

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    다국어 초록 (Multilingual Abstract) kakao i 다국어 번역

    The Argonne National Laboratory of the United States and the Kharkov Institute of Physicsand Technology of the Ukraine have been collaborating on the design, development andconstruction of a neutron source facility at Kharkov Institute of Physics and Technologyutilizing an electron-accelerator-driven subcritical assembly. The electron beam power is100 kW using 100-MeV electrons. The facility was designed to perform basic and appliednuclear research, produce medical isotopes, and train nuclear specialists. Thebiological shield of the accelerator building was designed to reduce the biological dose to lessthan 5.0e-03 mSv/h during operation. The main source of the biological dose for the acceleratorbuilding is the photons and neutrons generated from different interactions of leakedelectrons from the electron gun and the accelerator sections with the surrounding componentsand materials. The Monte Carlo N-particle extended code (MCNPX) was used for theshielding calculations because of its capability to perform electron-, photon-, and neutroncoupledtransport simulations. The photon dose was tallied using the MCNPX calculation,starting with the leaked electrons. However, it is difficult to accurately tally the neutron dosedirectly from the leaked electrons. The neutron yield per electron from the interactions withthe surrounding components is very small, ~0.01 neutron for 100-MeV electron and evensmaller for lower-energy electrons. This causes difficulties for the Monte Carlo analyses andconsumes tremendous computation resources for tallying the neutron dose outside theshield boundary with an acceptable accuracy. To avoid these difficulties, the SOURCE andTALLYXuser subroutines ofMCNPXwere utilized for this study.The generated neutrons werebanked, together with all related parameters, for a subsequent MCNPX calculation to obtainthe neutron dose. The weight windows variance reduction technique was also utilized forboth neutron and photon dose calculations. Two shielding materials, heavy concrete andordinary concrete, were considered for the shield design. The main goal is to maintain thetotal dose outside the shield boundary less than 5.0e-03 mSv/h during operation. The shieldconfiguration and parameters of the accelerator building were determined and are presentedin this paper.
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    The Argonne National Laboratory of the United States and the Kharkov Institute of Physicsand Technology of the Ukraine have been collaborating on the design, development andconstruction of a neutron source facility at Kharkov Institute of Physics and ...

    The Argonne National Laboratory of the United States and the Kharkov Institute of Physicsand Technology of the Ukraine have been collaborating on the design, development andconstruction of a neutron source facility at Kharkov Institute of Physics and Technologyutilizing an electron-accelerator-driven subcritical assembly. The electron beam power is100 kW using 100-MeV electrons. The facility was designed to perform basic and appliednuclear research, produce medical isotopes, and train nuclear specialists. Thebiological shield of the accelerator building was designed to reduce the biological dose to lessthan 5.0e-03 mSv/h during operation. The main source of the biological dose for the acceleratorbuilding is the photons and neutrons generated from different interactions of leakedelectrons from the electron gun and the accelerator sections with the surrounding componentsand materials. The Monte Carlo N-particle extended code (MCNPX) was used for theshielding calculations because of its capability to perform electron-, photon-, and neutroncoupledtransport simulations. The photon dose was tallied using the MCNPX calculation,starting with the leaked electrons. However, it is difficult to accurately tally the neutron dosedirectly from the leaked electrons. The neutron yield per electron from the interactions withthe surrounding components is very small, ~0.01 neutron for 100-MeV electron and evensmaller for lower-energy electrons. This causes difficulties for the Monte Carlo analyses andconsumes tremendous computation resources for tallying the neutron dose outside theshield boundary with an acceptable accuracy. To avoid these difficulties, the SOURCE andTALLYXuser subroutines ofMCNPXwere utilized for this study.The generated neutrons werebanked, together with all related parameters, for a subsequent MCNPX calculation to obtainthe neutron dose. The weight windows variance reduction technique was also utilized forboth neutron and photon dose calculations. Two shielding materials, heavy concrete andordinary concrete, were considered for the shield design. The main goal is to maintain thetotal dose outside the shield boundary less than 5.0e-03 mSv/h during operation. The shieldconfiguration and parameters of the accelerator building were determined and are presentedin this paper.

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    참고문헌 (Reference)

    1 Z. Zhong, "Shielding design and analysis of KIPT neutron source facility" 53 : 92-, 2011

    2 Y. S. Min, "Shielding Design for the Target Room of the Proton Accelerator Research Center" 한국물리학회 56 (56): 1971-1980, 2010

    3 Y.O. Lee, "Shielding Aspect of High Current Proton Linear Accelerator (KOMAC)" 2003

    4 S. Ohnishi, "Radiation shielding design for IFMIF/EVEDA accelerator vault" 9 : 190-192, 2010

    5 Z. Zhong, "Neutron Source in the MCNPX Shielding Calculation for Electron Driven Facility, Physor 2012"

    6 Denise B. Pelowitz, "MCNPX.2.7.B Extension"

    7 M.B. Chadwick, "ENDF/B-VII.0: next generation evaluated nuclear data library for nuclear science and technology" 107 : 2932-3061, 2006

    8 International Commission on Radiological Protection, "Conversion Coefficients for Use in Radiological Protection Against External Radiation"

    9 R. G. Williams, "Compendium of Material Composition Data for Radiation Transport Modeling"

    10 Z. Zhong, "Biological shield design and analysis of KIPT accelerator driven-subcritical facility" 168 : 871-, 2009

    1 Z. Zhong, "Shielding design and analysis of KIPT neutron source facility" 53 : 92-, 2011

    2 Y. S. Min, "Shielding Design for the Target Room of the Proton Accelerator Research Center" 한국물리학회 56 (56): 1971-1980, 2010

    3 Y.O. Lee, "Shielding Aspect of High Current Proton Linear Accelerator (KOMAC)" 2003

    4 S. Ohnishi, "Radiation shielding design for IFMIF/EVEDA accelerator vault" 9 : 190-192, 2010

    5 Z. Zhong, "Neutron Source in the MCNPX Shielding Calculation for Electron Driven Facility, Physor 2012"

    6 Denise B. Pelowitz, "MCNPX.2.7.B Extension"

    7 M.B. Chadwick, "ENDF/B-VII.0: next generation evaluated nuclear data library for nuclear science and technology" 107 : 2932-3061, 2006

    8 International Commission on Radiological Protection, "Conversion Coefficients for Use in Radiological Protection Against External Radiation"

    9 R. G. Williams, "Compendium of Material Composition Data for Radiation Transport Modeling"

    10 Z. Zhong, "Biological shield design and analysis of KIPT accelerator driven-subcritical facility" 168 : 871-, 2009

    11 C. N. Culbertson, "An Assessment of the MCNP4C Weight Window"

    12 Y. Gohar, "Accelerator-driven sub-critical facility: conceptual design development" 562 : 870-874, 2006

    13 R. L. Walker, "A Summary of Shielding Constant for Concrete"

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    연월일 이력구분 이력상세 등재구분
    2023 평가 해외DB학술지평가 신청대상 (해외등재 학술지 평가)
    2020-01-01 등재 등재학술지 유지 (해외등재 학술지 평가) KCI등재
    2014-01-01 등재 SCIE 등재 (등재유지) KCI등재
    2014-01-01 등재 SCOPUS 등재 (등재유지) KCI등재
    2011-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2009-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2007-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2006-07-31 학술지명변경 한글명 : Jorunal of the Korean Nuclear Society -> Nuclear Engineering and Technology
    외국어명 : 미등록 -> Nuclear Engineering and Technology
    KCI등재후보
    2004-01-01 등재 등재후보학술지 선정 (신규평가) KCI등재후보
    2003-01-01 등재 등재후보 1차 PASS (등재후보1차) KCI등재후보
    2002-01-01 등재 등재후보학술지 유지 (등재후보1차) KCI등재후보
    1999-01-01 등재 등재후보학술지 선정 (신규평가) KCI등재후보
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    기준연도 WOS-KCI 통합IF(2년) KCIF(2년) KCIF(3년)
    2016 1.04 0.17 0.77
    KCIF(4년) KCIF(5년) 중심성지수(3년) 즉시성지수
    0.63 0.56 0.343 0.11
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