• 제목/요약/키워드: Secondary jet

검색결과 164건 처리시간 0.03초

다양한 벽면 두께를 갖는 원형 노즐에서 분사되는 난류 충돌 및 벽면 제트 유동장 특성 (Characteristics of Turbulent Impinging and Wall Jet Flow for a Circular Nozzle with Various Exit Wall Thickness)

  • 양근영;윤상헌;손동기;최만수
    • 대한기계학회논문집B
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    • 제25권6호
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    • pp.751-757
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    • 2001
  • An experimental study of impinging jet-flow structure has been carried out for a fully developed single circular jet impingement cooling on a flat plate, and the effect of the wall thickness at nozzle exit edge is investigated. Impinging jet flow structures have been measured by Laser-Doppler Velocimeter to interpret the heat transfer results presented previously by Yoon et al.(sup)(10) The peaks of heat transfer rate are observed near the nozzle edge owing to the radial acceleration of jet flow when the nozzle locates close to the impingement plate. The growth of the velocity fluctuations in the wall jet flow is induced by the vortices which originate in the jet shear layer, and consequently the radial distribution of local Nusselt numbers has a secondary peak at the certain radial position. As a wall of circular pipe nozzle becomes thicker for small nozzle-to-target distance, the entrainment can be inhibited, consequently, the acceleration of wall jet flow is reduced and the heat transfer rate decreases.

고압실 형상에 따른 환형 제트펌프의 특성 (The Effect of High Pressure Chamber's Shape on the Characteristics of Annular Jet Pump)

  • 권오붕
    • 수산해양기술연구
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    • 제35권4호
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    • pp.428-434
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    • 1999
  • Experimental studies on the characteristics of annular jet pump were carried out in this paper. Jet pump can be used widely for the transportation of solid materials, farm produce and fishes. The effects of high pressure chamber on the characteristics of annular jet pump were sought in this paper. Experiments were done for three shapes of high pressure chamber, and for several lengths of the high pressure chamber. Three types of the high pressure chamber's entrances($90^{\circ}$ single inflow, $45^{\circ}$single inflow, and $45^{\circ}$ double inflow) were tested. Water was used for both the primary fluid and secondary fluid. The results obtained in this study are as follows; $45^{\circ}$double inflow type is the most effective among the tested three types of the high pressure chamber's entrances. The efficiency of jet pump with 400mm of high pressure chamber length is the highest among the chamber lengths tested in this study, thus indicating appropriate chamber length is required to get an efficient.

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피스톤 냉각용 Oil Jet 유동 수치해석 (A Numerical investigation of Oil Jet in an Engine Piston)

  • 리리;권지혁;정호윤;최윤환;이연원
    • 한국마린엔지니어링학회:학술대회논문집
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    • 한국마린엔지니어링학회 2005년도 후기학술대회논문집
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    • pp.33-34
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    • 2005
  • The internal state of an automotive engine is very severe. A piston exposes burnt gas of over $2000^{\circ}$ nd is shocked by high pressure at the time of explosion. Furthermore strong friction is caused by high speed motion. A study on the cooling of the piston requires because the cooling and lubrication of the piston has an effect on the life and efficiency of engine directly. The previous system of oil jet cooled only the bottom of the piston. In order to improve the cooling efficiency, the oil gallery is made inside the piston, and oil flows into the oil gallery. The flow rate of oil at the entrance of oil gallery is important because of the cooling efficiency. The purpose of this study is the investigation of fluid flow characteristics of oil jet and flow rate into the oil gallery.

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평면제트를 이용한 충돌면에서의 난류유동 특성 (Turbulent Flow Characteristics using Plane Jet on Impingement Surface)

  • 윤순현
    • Journal of Advanced Marine Engineering and Technology
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    • 제22권4호
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    • pp.429-435
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    • 1998
  • Experiments were conducted to investigate the turbulent flow characteristics from on oblique impingement surface to an plane jet at the jet Reynolds number(Re based on the nozzle width) $3{\times}10^4$ The jet mean velocity and turbulent intensity profiles have been measured along the impingement surface by hot-wire anemometer. The nozzle-to-plate distance(H/B) ranged from 2 to 10 and the oblique angle (a) from 45 to 90 degree. Also the secondary peak of the turbulent intensity was observed at H/B=4 S/B 5 and a=90 degree. It has been found that the stagnation point shifted toward the minor flow region as the oblique angle decreased and the position of the stagnation point nearly coincided with that of the maximum turbulent intensity.

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원형 노즐의 직경 변화 및 표면으로 부터의 거리변화에 따른 오목한 표면에 충돌하는 제트의 온도장 측정 및 CFD해석 (Temperature field measurement and CFD analysis of a jet impinging on a concave surface depending on changes in nozzle to surface distance and the diameter of a circular nozzle)

  • 조영민;임유진;염은섭
    • 한국가시화정보학회지
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    • 제21권2호
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    • pp.55-62
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    • 2023
  • The characteristic of jet impinging on the concave surface were analyzed through thermographic phosphor thermometry (TPT) and numerical investigation. Under a jet Reynolds number of 6600, nozzle diameters and nozzle-to-surface distances (H/d) were changed 5mm and 10mm and H/d=2 and 5. The RNG k-ε turbulence model can accurately predict the distribution of Nusselt number, compared to other models (SST k-ω, realizable k-ε). Heat transfer characteristics varied with the nozzle diameter and H/d, with a secondary peak noted at H/d =2, due to vortex-induced flow detachment and reattachment. An increase in nozzle diameter enhanced jet momentum, turbulence strength, and heat transfer.

Experimental investigation of jet pump performance used for high flow amplification in nuclear applications

  • Vimal Kotak;Anil Pathrose;Samiran Sengupta;Sugilal Gopalkrishnan;Sujay Bhattacharya
    • Nuclear Engineering and Technology
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    • 제55권10호
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    • pp.3549-3558
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    • 2023
  • The jet pump can be used in a test device of a nuclear reactor for high flow amplification as it reduces inlet flow requirement and thereby size of the process components. In the present work, a miniature jet pump was designed to meet high flow amplification greater than 3. Subsequently, experiments were carried out using a test setup for design validation and performance evaluation of the jet pump for different parameters. It was observed that a minimum pressure of 0.6 bar (g) was required for the secondary fluid inside the jet pump to ensure cavitation free performance at high amplification. Spacing between the nozzle tip and the mixing chamber entry point had significant effect on the performance of the jet pump. Variation in primary flow, temperature and area ratio also affected the performance. It was observed that at high flow amplification, the analytical solution differed significantly from experimental results due to very large velocities encountered in the miniature size jet pump.

음속 이차유동 분출시 나타나는 초음속 노즐 내부 유동장에 관한 연구 (Study of Flowfield of the Interaction of Secondary Sonic Jet into a Supersonic Nozzle)

  • 고현;이열;윤웅섭
    • 한국추진공학회지
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    • 제7권3호
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    • pp.45-52
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    • 2003
  • 원추형 초음속 노즐 확산부에 이차유동이 음속으로 분출될 때 나타나는 노즐 내부 유동장에 대한 수치적 연구가 이루어졌다. 대수-난류모델과 $\kappa$-$\varepsilon$ 모델을 사용한 레이놀즈-평균 Navier-Stokes 방정식을 계산함으로서 노즐 내부에서 나타나는 충격파와 경계층의 간섭에 의한 3 차원 유동장을 해석하였다. 얻어진 수치해석의 결과는 동일한 조건에서 수행된 실험결과와 잘 일치하고 있음이 판명되었다. 이차유동의 분출압력 변화가 충격파와 경계층의 간섭과 함께 노즐내부 유동장 구조에 미치는 영향을 평가하였다. 아울러 충격파 간섭 후방에서 나타나는 와류유동 구조와 벽면 압력분포에 관한 정보를 얻었다.

초음속 유동장내 2차분사 분사각도 변화에 따른 열전달 특성 변화 (Heat Transfer on Secondary Injection Surface in Supersonic Flow-field with Various Injection Angle)

  • 송지운;이종주;조형희;배주찬
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2008년도 제31회 추계학술대회논문집
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    • pp.321-325
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    • 2008
  • 초음속 유동장내에 분사된 2차제트 주변에서의 열전달 현상을 고찰 하였다. 초음속 유동장내에 분사되는 2차유동의 Jet to freestream momentum ratio(운동량비)의 변화와, 2차유동 분사각도에 따른 2차 분사홀 주변의 열전달 특성을 파악하기 위하여 홀 주변의 표면온도 변화를 고속 적외선 카메라를 통하여 측정하였으며, 이를 이용하여 비정상 열유속 기법을 바탕으로 열유속을 계산하였다. 운동량비가 증가할 수록 열전달 현상이 강화 되었으며, $15^{\circ}$ 기울어진 분사보다는 수직 분사의 경우에 더 강한 열전달 현상이 발생되었다. 이를 통해 분사비와 분사 각도가 표면 열전달 분포에 중요한 요인으로 작용함을 확인할 수 있었다.

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볼록한 반구면에 충돌하는 원형제트의 열전달 및 유동특성 (Heat transfer and flow characteristics of a circular jet impinging on a convex curved surface)

  • 이대희;정영석;임경빈;김대성
    • 대한기계학회논문집B
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    • 제21권4호
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    • pp.579-588
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    • 1997
  • The heat transfer and flow measurements from a convex curved surface to a circular impinging jet have been made. The flow at the nozzle exit has a fully developed velocity profile. The jet Reynolds number (Re) ranges from 11,000 to 50,000, the dimensionless nozzle-to-surface distance (L/d) from 2 to 10, and the dimensionless surface curvature (d/D) from 0.034 to 0.089. The results show that the stagnation point Nusselt number (N $u_{st}$ ) increases with increasing value of d/D. The maximum Nusselt number at the stagnation point occurs at L/d .ident. 6 to 8 for all Re's and d/D's tested. For larger L/d, N $u_{st}$ dependency on Re is stronger due to an increase of turbulence in the approaching jet as a result of the more active exchange of momentum with a surrounding air. The local Nusselt number decreases monotonically from its maximum value at the stagnation point. However, for L/d=2 and Re=23,000, and for L/d.leq.4 and Re=50,000, the stream wise Nusselt number distributions exhibit secondary maxima at r/d .ident. 2.2. The formation of the secondary maxima is attributed to an increase in the turbulence level resulting from the transition from a laminar to a turbulent boundary layer.ndary layer.

충돌제트를 이용한 Pedestal 형상의 칩 냉각연구 (Jet Impingement Heat Transfer on a Cylindrical Pedestal Encountered in Chip Cooling)

  • 이대희;이준식;정영석;정승훈
    • 대한기계학회논문집B
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    • 제27권1호
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    • pp.1-8
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    • 2003
  • The heat transfer and flow measurements on a cylindrical pedestal mounted on a flat surface with a turbulent impinging jet were made. The experiments were made for the jet Reynolds number of Re = 23,000, the dimensionless nozzle-to-surface distance of L/d = 2~10, the dimensionless pedestal height of H/D = 0~1.5. Measurements of the surface temperature and the Nusselt number distributions on the plate surface were made using liquid crystal and shroud-transient technique. Flow measurements involve smoke flow visualization and the wall pressure coefficient. The results show that the wall pressure coefficient sharply decreases along the upper surface of the pedestal. However, the pressure increases when the fluid escapes from the pedestal and then collides on the plate surface. The secondary maxima in the Nusselt numbers occur in the region of 1.0 $\leq$ r/d $\leq$ 1.9. Their values for the case of H/D = 0.5 are maximum 80% higher than those for other cases. The formation of the secondary maxima may be attributed to the reattachment of flow on the plate surface which was separated at the edge of the pedestal.