• 제목/요약/키워드: Thermal Plume Interaction

검색결과 5건 처리시간 0.014초

로켓엔진 병렬화에 의한 저부가열의 수치적 예측 (Numerical Prediction of the Base Heating due to Rocket Engine Clustering)

  • 김성룡;김인선
    • 한국전산유체공학회지
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    • 제9권3호
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    • pp.18-25
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    • 2004
  • Multi plume effects on the base heating have been Investigated with a CFD program. As the flight altitude increases, the plume expansion angle increases regardless of the single or clustered engine. The plume interaction of the clustered engine makes a high temperature thermal shear in the center of four plumes. At low altitude, the high temperature shear flow stays in the center of plumes, but it increases up to engine base with the increasing altitude. At high altitude, the flow from plume to base and the flow from base into outer free stream are supersonic, which transfers the high heat in the center of plumes to the base region. The radiative heat of the clustered engine varies from 220 kW/m² to 469 kW/m² with increasing altitude while those of the single engine are 10 kW/m² and 43.7 kW/m². And the base temperature of the clustered engine varies from 985K to 1223K, and those of the single engine are 483K and 726K. This big radiative heat of clustered engine can be explained by the active high temperature base flow and strong plume interactions.

등온 수직 평판에서의 혼합대류 열전달 (Mixed convection from two isothermal, vertical, parallel plates)

  • 박문길;이재신;양성환;권순석
    • 대한기계학회논문집
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    • 제14권6호
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    • pp.1645-1651
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    • 1990
  • 본 연구에서는 두 개의 수직 등온 평판이 평행하게 배열된 경우의 혼합대류 열전달에 대하여 무차원 평판 간격, b/l와 Grashof수, 레이놀즈수를 변수로 유한차분 법을 사용 수치해석하고, 두평판사잉의 간섭현상과 열전달을 최대로 하는 최적 평판간 격을 구하였다.

외부 직각모서리 부근에서의 자연대류 열전달 (Natural Convection Heat Transfer Past an Outer Rectangular Corner)

  • 신순철;장근식;김승수
    • 대한기계학회논문집
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    • 제9권5호
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    • pp.598-605
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    • 1985
  • 본 논문에서는 공기(Pr*0.72) 중에서 등온으로 가열된 유한한 길이의 수평평 판과 수직평판이 직각을 이루는 경우의 2차원 유동 및 열전달 현상을 G $r_{LH}$ <1.25 $\times$$10^{6}$인 층류영역에서 고찰하였다.수평부위 및 수직부위로 부터 발생하는 평 면 열상승류(Plume)의 상호작용에 의해 독립된 각 평판에 대한 상사해 및 실험과는 다 른 결과를 얻을 수 있었고 이들을 온도장(temperature field)의 변화 및 국소 열유속 의 변화에 촛점을 맞추어 해석하였다. 또한 Nusselt수를 Grashof수와, 수평부위와 수직부위의 종횡비에 대해 정리하였는데 보다 일반적인 종횡비에 대해서도 해석이 가 능하도록 이 형상에 대한 새로운 특성길이를 제시하였다.이상의 실험을 위해서는 Mach-Zehnder 간섭계(MZI)를 사용하였다.

수직으로 엇갈린 등온평판에서의 혼합대류 열전도 (Mixed Convection Heat Transfer from Vertically Misaligned Isothermal plates)

  • 권순석;김상영;박순업
    • 한국해양공학회지
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    • 제6권1호
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    • pp.52-61
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    • 1992
  • The steady laminar mixed convection from vertically misaligned, isothermal plastes has been studied by numerical procedure. The governing equations are solved by the finite difference method using successive using successive over relaxation scheme at Re=100-800, $Gr=10^3-10^6$, Pr=0.71 and dimensionless plate spacings b/L=0.1-1.0. The plume interaction caused by the thermal interference of twoplates is observed. As Reynolds numbers increase, the optimum plate spacings are moved to narrow spacings at the same Grashof number and as Grashof numbers increase, to wide spacings at the same Reynolds number.

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이동식 미분무수 노즐의 소화 특성에 대한 수치 시뮬레이션 (Thermal Numerical Simulation on Fire Suppression Characteristics through Mobile Mist Spray Nozzles)

  • 배강열;정희택;김형범;정인수;김창
    • 동력기계공학회지
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    • 제13권5호
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    • pp.25-33
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    • 2009
  • In the present study, the numerical investigation has been carried out to see the effects of water mist sprays on the fire suppression mechanism. The special-purposed program named as FDS was used to simulate the interaction of fire plume and water mists. This program solves the fire-driven flows using LES turbulence model, the mixture fraction combustion model, the finite volume method of radiation transport for a non-scattering gray gas, and conjugate heat transfer between wall and gas flow. The computational domain was composed of a rectangular space dimensioned as $L{\times}W{\times}H=4.0{\times}4.0{\times}2.5\;m^3$ with a mist-injecting nozzle installed 1.0 m high from the fire pool. In this paper, two types of nozzles were chosen to compare the performance of the fire suppression. Numerical results showed that the nozzle, type A, with more orifices having smaller diameters had poorer performance than the other one, type B because the flow injected through side holes deteriorated the primary flow. The fire-extinguishing time of type A was 2.6 times bigger than that of type B.

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