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      https://www.riss.kr/link?id=A60198241

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      다국어 초록 (Multilingual Abstract) kakao i 다국어 번역

      Direct Numerical Simulation(DNS) of turbulent mass transfer in fully developed turbulent pipe flow has been performed to study the effect of wall boundary conditions on the concentration fields at Re<SUB>τ</SUB>=180 based on friction velocity and pipe radius. Fully developed turbulent pipe flows for Sc=0.71 are studied with two different wall boundary conditions, namely, constant mass flux and constant wall concentration. The mean concentration profiles and turbulent mass fluxes obtained from the present DNS are in good agreement with the previous numerical results currently available. To investigate the effects of wall boundary condition on the turbulent mass transfer, the mean concentration profile, root-mean-square of concentration fluctuation, turbulent mass fluxes and higher-order statistics(Skewness and Flatness factor) are compared for the two cases. Furthermore, the budgets of turbulent mass fluxes and concentration variance were computed and analyzed to elucidate the effects of wall boundary conditions on the turbulent mass transfer.
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      Direct Numerical Simulation(DNS) of turbulent mass transfer in fully developed turbulent pipe flow has been performed to study the effect of wall boundary conditions on the concentration fields at Re<SUB>τ</SUB>=180 based on friction velo...

      Direct Numerical Simulation(DNS) of turbulent mass transfer in fully developed turbulent pipe flow has been performed to study the effect of wall boundary conditions on the concentration fields at Re<SUB>τ</SUB>=180 based on friction velocity and pipe radius. Fully developed turbulent pipe flows for Sc=0.71 are studied with two different wall boundary conditions, namely, constant mass flux and constant wall concentration. The mean concentration profiles and turbulent mass fluxes obtained from the present DNS are in good agreement with the previous numerical results currently available. To investigate the effects of wall boundary condition on the turbulent mass transfer, the mean concentration profile, root-mean-square of concentration fluctuation, turbulent mass fluxes and higher-order statistics(Skewness and Flatness factor) are compared for the two cases. Furthermore, the budgets of turbulent mass fluxes and concentration variance were computed and analyzed to elucidate the effects of wall boundary conditions on the turbulent mass transfer.

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      참고문헌 (Reference)

      1 Antonia, R.A, "Turbulent Prandtl number in the near-wall region of a turbulent channel flow" 34 (34): 1905-1908, 1991

      2 Kim, J, "Turbulence statics in fully developed channel flow at low Reynolds number" 177 : 133-166, 1987

      3 Saha, S, "The influence of pipe length on thermal statistics computedfrom DNS of turbulent heat transfer" 32 : 1083-1097, 2011

      4 Kader, B.A, "Temperature and concentration profiles in fully turbulent boundary layers" 24 (24): 1541-1544, 1981

      5 Eggels, J.G.M, "Fully developed turbulent pipe flow : a comparison between direct numerical simulation and experiment" 268 : 175-209, 1994

      6 Redjem-Saad, L., "Direct numerical simulation of turbulent heat transfer inpipe flows: Effect of Prandtl number" 28 : 847-861, 2007

      7 Satake, S, "Direct numerical simulation of turbulent heat transfer in an axially rotating pipe flow; Reynolds shear stress and scalar flux budgets" 12 (12): 958-1008, 2002

      8 Piller, M, "Direct numerical simulation of turbulent forced convection in a pipe" 49 : 583-602, 2005

      9 Kasagi, N, "Direct numerical simulation of passive scalar field in a turbulent channel flow" 114 : 598-606, 1992

      10 Kawamura, H, "DNS of turbulent heat transfer in channel flow with respect to Reynolds and Prandtl number effects" 20 : 196-207, 1999

      1 Antonia, R.A, "Turbulent Prandtl number in the near-wall region of a turbulent channel flow" 34 (34): 1905-1908, 1991

      2 Kim, J, "Turbulence statics in fully developed channel flow at low Reynolds number" 177 : 133-166, 1987

      3 Saha, S, "The influence of pipe length on thermal statistics computedfrom DNS of turbulent heat transfer" 32 : 1083-1097, 2011

      4 Kader, B.A, "Temperature and concentration profiles in fully turbulent boundary layers" 24 (24): 1541-1544, 1981

      5 Eggels, J.G.M, "Fully developed turbulent pipe flow : a comparison between direct numerical simulation and experiment" 268 : 175-209, 1994

      6 Redjem-Saad, L., "Direct numerical simulation of turbulent heat transfer inpipe flows: Effect of Prandtl number" 28 : 847-861, 2007

      7 Satake, S, "Direct numerical simulation of turbulent heat transfer in an axially rotating pipe flow; Reynolds shear stress and scalar flux budgets" 12 (12): 958-1008, 2002

      8 Piller, M, "Direct numerical simulation of turbulent forced convection in a pipe" 49 : 583-602, 2005

      9 Kasagi, N, "Direct numerical simulation of passive scalar field in a turbulent channel flow" 114 : 598-606, 1992

      10 Kawamura, H, "DNS of turbulent heat transfer in channel flow with respect to Reynolds and Prandtl number effects" 20 : 196-207, 1999

      11 Kawamura, H., "DNS of turbulent heat transfer in channel flow with low to medium-high Prandtl number fluid" 19 : 482-491, 1998

      12 Bejan, A., "Convection Heat Transfer" Wiley 2004

      13 Kim, J., "Application of a fractional-step method to incompressible Navier-Stokes equations" 59 : 308-323, 1985

      14 Akselvoll, K., "An efficient method for temporal integration of the Navier-Stokes equation in confined axisymmetric geometries" 125 : 454-463, 1996

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      학술지 이력

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