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    다국어 초록 (Multilingual Abstract) kakao i 다국어 번역

    Recently, researchers have developed simple lattice Boltzmann method without evolution of distribution functions. The method has an advantage that physical boundary conditions can be implemented directly. Taking the advantage, we implement a convection boundary scheme to the simple lattice Boltzmann method. This boundary scheme is derived from an assumption that the convection heat flux is equal to the conduction heat flux. Then, the heat transfer coefficient can be expressed by the thermal conductivity. Using the coefficients, the wall temperature is set directly on the boundary condition of simple lattice Boltzmann method unlike convectional lattice Boltzmann method. For verifications and validations, we apply our scheme to three cases in a row. First of all, we compute a natural convection in a square cavity for validation of simple lattice Boltzmann method. Secondly, the convection boundary scheme is applied to steady one-dimension heat conduction on a solid. Lastly, we simulate a square cavity with the convection boundary scheme. In this case, we assume that the boundary is thin. Our result is compared with commercial solver, FLUENT. The results show that the convection boundary scheme used in this study can be applied to the simple lattice Boltzmann method.
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    Recently, researchers have developed simple lattice Boltzmann method without evolution of distribution functions. The method has an advantage that physical boundary conditions can be implemented directly. Taking the advantage, we implement a convectio...

    Recently, researchers have developed simple lattice Boltzmann method without evolution of distribution functions. The method has an advantage that physical boundary conditions can be implemented directly. Taking the advantage, we implement a convection boundary scheme to the simple lattice Boltzmann method. This boundary scheme is derived from an assumption that the convection heat flux is equal to the conduction heat flux. Then, the heat transfer coefficient can be expressed by the thermal conductivity. Using the coefficients, the wall temperature is set directly on the boundary condition of simple lattice Boltzmann method unlike convectional lattice Boltzmann method. For verifications and validations, we apply our scheme to three cases in a row. First of all, we compute a natural convection in a square cavity for validation of simple lattice Boltzmann method. Secondly, the convection boundary scheme is applied to steady one-dimension heat conduction on a solid. Lastly, we simulate a square cavity with the convection boundary scheme. In this case, we assume that the boundary is thin. Our result is compared with commercial solver, FLUENT. The results show that the convection boundary scheme used in this study can be applied to the simple lattice Boltzmann method.

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    참고문헌 (Reference)

    1 Chen, Z., "Three-dimensional simplified and unconditionally stable lattice Boltzmann method for incompressible isothermal and thermal flows" 29 (29): 053601-, 2017

    2 Chen, Z, "Highly accurate simplified lattice Boltzmann method" 30 (30): 103605-, 2018

    3 Chen, Z., "High-order simplified thermal lattice Boltzmann method for incompressible thermal flows" 127 : 1-16, 2018

    4 d’Humieres, A., "Generalized Lattice-Boltzmann Equations" 159 : 450-458, 1992

    5 d’Orazio, A, "Boundary Conditions for Thermal Lattice Boltzmann Simulations" 977-986, 2003

    6 Chen, Z., "A simplified thermal lattice Boltzmann method without evolution of distribution functions" 105 : 741-757, 2017

    7 Chen, Z., "A Simplified Lattice boltzmann Method without Evolution of Distribution Function" 9 (9): 1-22, 2017

    1 Chen, Z., "Three-dimensional simplified and unconditionally stable lattice Boltzmann method for incompressible isothermal and thermal flows" 29 (29): 053601-, 2017

    2 Chen, Z, "Highly accurate simplified lattice Boltzmann method" 30 (30): 103605-, 2018

    3 Chen, Z., "High-order simplified thermal lattice Boltzmann method for incompressible thermal flows" 127 : 1-16, 2018

    4 d’Humieres, A., "Generalized Lattice-Boltzmann Equations" 159 : 450-458, 1992

    5 d’Orazio, A, "Boundary Conditions for Thermal Lattice Boltzmann Simulations" 977-986, 2003

    6 Chen, Z., "A simplified thermal lattice Boltzmann method without evolution of distribution functions" 105 : 741-757, 2017

    7 Chen, Z., "A Simplified Lattice boltzmann Method without Evolution of Distribution Function" 9 (9): 1-22, 2017

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    학술지 이력

    학술지 이력
    연월일 이력구분 이력상세 등재구분
    2027 평가 재인증평가 신청대상 (재인증)
    2021-01-01 등재 등재학술지 유지 (재인증) KCI등재
    2018-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2015-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2011-01-01 등재 등재 1차 FAIL (등재유지) KCI등재
    2009-01-01 등재 등재학술지 유지 (등재유지) KCI등재
    2006-01-01 등재 등재학술지 선정 (등재후보2차) KCI등재
    2005-06-16 학술지명변경 외국어명 : Jpurnal of Computatuonal Fluids Engineering -> Korean Society of Computatuonal Fluids Engineering KCI등재후보
    2005-01-01 등재 등재후보 1차 PASS (등재후보1차) KCI등재후보
    2004-01-01 등재 등재후보 1차 FAIL (등재후보1차) KCI등재후보
    2002-07-01 등재 등재후보학술지 선정 (신규평가) KCI등재후보
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    학술지 인용정보

    학술지 인용정보
    기준연도 WOS-KCI 통합IF(2년) KCIF(2년) KCIF(3년)
    2016 0.2 0.2 0.19
    KCIF(4년) KCIF(5년) 중심성지수(3년) 즉시성지수
    0.16 0.15 0.405 0.05
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