• 제목/요약/키워드: CFD code

검색결과 974건 처리시간 0.023초

Heat transfer analysis in sub-channels of rod bundle geometry with supercritical water

  • Shitsi, Edward;Debrah, Seth Kofi;Chabi, Silas;Arthur, Emmanuel Maurice;Baidoo, Isaac Kwasi
    • Nuclear Engineering and Technology
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    • 제54권3호
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    • pp.842-848
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    • 2022
  • Parametric studies of heat transfer and fluid flow are very important research of interest because the design and operation of fluid flow and heat transfer systems are guided by these parametric studies. The safety of the system operation and system optimization can be determined by decreasing or increasing particular fluid flow and heat transfer parameter while keeping other parameters constant. The parameters that can be varied in order to determine safe and optimized system include system pressure, mass flow rate, heat flux and coolant inlet temperature among other parameters. The fluid flow and heat transfer systems can also be enhanced by the presence of or without the presence of particular effects including gravity effect among others. The advanced Generation IV reactors to be deployed for large electricity production, have proven to be more thermally efficient (approximately 45% thermal efficiency) than the current light water reactors with a thermal efficiency of approximately 33 ℃. SCWR is one of the Generation IV reactors intended for electricity generation. High Performance Light Water Reactor (HPLWR) is a SCWR type which is under consideration in this study. One-eighth of a proposed fuel assembly design for HPLWR consisting of 7 fuel/rod bundles with 9 coolant sub-channels was the geometry considered in this study to examine the effects of system pressure and mass flow rate on wall and fluid temperatures. Gravity effect on wall and fluid temperatures were also examined on this one-eighth fuel assembly geometry. Computational Fluid Dynamics (CFD) code, STAR-CCM+, was used to obtain the results of the numerical simulations. Based on the parametric analysis carried out, sub-channel 4 performed better in terms of heat transfer because temperatures predicted in sub-channel 9 (corner subchannel) were higher than the ones obtained in sub-channel 4 (central sub-channel). The influence of system mass flow rate, pressure and gravity seem similar in both sub-channels 4 and 9 with temperature distributions higher in sub-channel 9 than in sub-channel 4. In most of the cases considered, temperature distributions (for both fluid and wall) obtained at 25 MPa are higher than those obtained at 23 MPa, temperature distributions obtained at 601.2 kg/h are higher than those obtained at 561.2 kg/h, and temperature distributions obtained without gravity effect are higher than those obtained with gravity effect. The results show that effects of system pressure, mass flowrate and gravity on fluid flow and heat transfer are significant and therefore parametric studies need to be performed to determine safe and optimum operating conditions of fluid flow and heat transfer systems.

RANS simulation of secondary flows in a low pressure turbine cascade: Influence of inlet boundary layer profile

  • Michele, Errante;Andrea, Ferrero;Francesco, Larocca
    • Advances in aircraft and spacecraft science
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    • 제9권5호
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    • pp.415-431
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    • 2022
  • Secondary flows have a huge impact on losses generation in modern low pressure gas turbines (LPTs). At design point, the interaction of the blade profile with the end-wall boundary layer is responsible for up to 40% of total losses. Therefore, predicting accurately the end-wall flow field in a LPT is extremely important in the industrial design phase. Since the inlet boundary layer profile is one of the factors which most affects the evolution of secondary flows, the first main objective of the present work is to investigate the impact of two different inlet conditions on the end-wall flow field of the T106A, a well known LPT cascade. The first condition, labeled in the paper as C1, is represented by uniform conditions at the inlet plane and the second, C2, by a flow characterized by a defined inlet boundary layer profile. The code used for the simulations is based on the Discontinuous Galerkin (DG) formulation and solves the Reynolds-averaged Navier-Stokes (RANS) equations coupled with the Spalart Allmaras turbulence model. Secondly, this work aims at estimating the influence of viscosity and turbulence on the T106A end-wall flow field. In order to do so, RANS results are compared with those obtained from an inviscid simulation with a prescribed inlet total pressure profile, which mimics a boundary layer. A comparison between C1 and C2 results highlights an influence of secondary flows on the flow field up to a significant distance from the end-wall. In particular, the C2 end-wall flow field appears to be characterized by greater over turning and under turning angles and higher total pressure losses. Furthermore, the C2 simulated flow field shows good agreement with experimental and numerical data available in literature. The C2 and inviscid Euler computed flow fields, although globally comparable, present evident differences. The cascade passage simulated with inviscid flow is mainly dominated by a single large and homogeneous vortex structure, less stretched in the spanwise direction and closer to the end-wall than vortical structures computed by compressible flow simulation. It is reasonable, then, asserting that for the chosen test case a great part of the secondary flows details is strongly dependent on viscous phenomena and turbulence.

교행식생 영역을 갖는 개수로 흐름에서의 3차원 수치모의 (Three-Dimensional Numerical Simulations of Open-Channel Flows with Alternate Vegetated Zones)

  • 강형식;김규호;임동균
    • 대한토목학회논문집
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    • 제29권3B호
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    • pp.247-257
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    • 2009
  • 본 연구에서는 흐름방향으로 식생 영역이 교차적으로 식재된 교행식생 수로에서의 3차원 수치모의를 수행하였다. 지배방정식에서의 난류 폐합을 위해 ${\kappa}-{\varepsilon}$ 모형을 적용하였으며, 수치모형은 Olsen(2004)이 개발한 3차원 모형을 이용하였다. 먼저, 3차원 수치모형을 이용하여 하상의 일부가 식재된 부분 식생 수로를 수치모의 하고, 계산된 적분유속 및 레이놀즈응력을 기존의 실험 결과와 비교하였다. 그 결과 본 모형이 식생 수로에서의 평균 유속 분포를 매우 잘 예측하는 것으로 나타났다. 그러나 ${\kappa}-{\varepsilon}$ 모형이 등방성 모형이므로 식생과 비식생 영역의 경계면 부근에서 발생되는 운동량 교환 효과를 정확히 예측할 수 없는 것으로 나타났다. 한편, 주흐름방향으로 식생 영역이 교차적으로 존재하는 교행식생 수로를 수치모의 하고, 계산된 유속 분포를 기존의 실험 결과와 비교한 결과, 계산 유속과 실험 결과가 매우 잘 일치하는 것으로 나타났다. 또한 다양한 밀도에 따른 유속 벡터도를 계산한 결과, 식생밀도가 증가함에 따라 식생이 흐름 방향을 변화 시켜 점차 만곡수로와 유사한 형태의 유속 벡터도를 갖는 것으로 나타났으며, 식생 밀도 ${\alpha}$가 9.97%인 경우에는 식생 반대 측벽 영역에서 재순환 흐름이 형성되는 것으로 나타났다. 한편, 식생 밀도에 따른 단면 유속 분포도 및 편수위 변화를 살펴보았다.

수중 무선 전화기의 설계 - 수중무선전화기 설계를 위한 수중소음분석을 중심으로- (The Design of Wireless Underwater Telephone -Analysis of Underwater Background Noise for Wireless Underwater Telephone Design -)

  • 박문갑;윤갑동;김석제;윤종락
    • 수산해양기술연구
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    • 제37권4호
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    • pp.302-307
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    • 2001
  • 본 연구는 잠수기 어업용 수중무선전화기를 설계하는데 있어 최적의 반송 주파수와 송신 신호의 음원 준위를 결정할 목적으로 우리 나라 잠수기 주 조업장의 하나인 거제와 통영 해역의 해양 배경소음과 조업중인 잠수기 어장의 수중 소음에 대하여 검토, 고찰한 결과를 요약하면 다음과 같다. 1. 거제와 통영의 잠수기 어장의 해양 배경 소음을 분석한 결과, 음압 준위는 25∼301kHz 부근에서 가장 낮아 52∼57dB이었고, 주변 통항 선박량과 산업시설이 많은 거제 해역이 통영 해역보다 약 5dB 더 높았다. 2. 거제와 통영의 잠수기 어선의 조업중의 수중소음을 비교하면, 최저 음압준위는 30kHz 부근에서 거제 어장에서는 67dB로서 통영의 62d묘보다 5dB 높은 음압 준위를 나타냈다. 이것은 거제 해역은 잠수기 어선의 규모도 통영 해역의 잠수기 어선보다 약간 크고, 분사기를 사용하여 작업하는데 비해 통영 해역은 잠수기 어선의 크기도 상대적으로 작고, 주 어획 대상물이 달라 분사기를 사용하지 않는 것이 그 원인으로 판단된다. 3. 거제 해역의 패류 채취용 분사기를 사용할 때의 수중 소음의 음압 준위는 102dB었다. 4. 거제 해역의 조업중에 대한 수중 배경 소음을 67dB라 가정할 때, 최대 500m까지 통화하기 위한 송신 신호의 음원 준위는 131dB 정도이다. 그러나, 통영 해역의 잠수기 조업은 분사기를 사용하지 않는 조업으로 이 경우 배경 소음은 약 62dB로서 송신 신호의 음원 준위는 126dB정도이다. 잠수기 조업중이 아닌 경우 즉, 스쿠버 다이버용 수중무선 전화기인 경우에는 배경 소음이 52∼57dB이므로 송신 신호의 음원 준위는 l16∼121dB이면 될 것으로 판단된다. 협동학습 모형이 수학 수업에 보다 발전적으로 널리 적용되기를 기대한다.cal results well visualized the streamlines, pressure fields, and speed vectors of a simple cambered and slot cambered otter board with slot size 0.02C. The slot cambered one with slot size 0.02C was shown that pressure field was distributed moderately on front and back side of otter board. And, the delay and decrease of separation were favorably achieved by flow through slot. 4. Computed result on the pattern of hydrodynamic field and the values of C/sub L/ and C/sub D/ by the commercial CFD code, FLUENT, show almost the same as those of the experimental result.erence was found in its fragrance. And, no difference was found in brightness and viscosity between samples. As a result of conducting the palatability test, no difference was showed in the appearance, but as for the overall palatability

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