• Title/Summary/Keyword: 피동제어

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A Study on the Reduction of Supersonic Cavity Pressure Oscillations Using a Sub-Cavity System (보조공동을 이용한 초음속 공동내부의 압력진동 저감에 관한 연구)

  • Shin, Choon-Sik;Jeong, June-Chang;Suryan, Abhilash;Kim, Heuy-Dong
    • Journal of the Korean Society of Propulsion Engineers
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    • v.13 no.5
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    • pp.41-47
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    • 2009
  • Numerical computations were carried out to analyze the effect of a sub-cavity at several inlet Mach numbers on the control of cavity-induced pressure oscillations in two-dimensional supersonic flow. The present passive control method, the sub-cavity applied to the front wall of a square cavity, was studied for the inlet Mach numbers of 1.50, 1.83 and 2.50. The results show that the sub-cavity is effective in reducing the oscillations, and a resultant amount of the reduction depended on the inlet Mach number, the length of flat plate, and the depth of sub-cavity used as an oscillation suppressor.

Experimental/Computational Study on the Supersonic Cavity Flow with a Sub-Cavity to Reduce the Pressure Oscillation (압력진동을 저감하기 위한 sub-cavity를 가진 초음속 공동유동에 대한 실험 및 수치해석적 연구)

  • Lim, Chae-Min;Lee, Young-Ki;Kim, Heuy-Dong
    • Proceedings of the KSME Conference
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    • 2007.05b
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    • pp.3009-3014
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    • 2007
  • The effectiveness of passive control techniques for alleviating the pressure oscillation generated in a supersonic cavity flow was investigated numerically and experimentally, respectively. The control device includes a sub-cavity installed near the leading edge of a rectangular cavity. Time-dependent supersonic cavity flow characteristics with turbulent features were examined by using the three-dimensional, mass-averaged Navier-Stokes computation based on a finite volume scheme and large eddy simulation. The results show that the pressure oscillation near the trailing edge dominates overall time-dependent cavity pressure variations. Such an oscillation can be attenuated more significantly in the presence of the sub-cavity compared with the cavity without sub-cavity, and a larger sub-cavity leads to better control performance.

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Passive Control for the Augmentation of a Pulse Wave (펄스파 강도증가를 위한 피동제어)

  • 이동훈;김희동;강성황
    • Journal of KSNVE
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    • v.11 no.2
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    • pp.241-248
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    • 2001
  • The present paper describes experimental and computational work to augment the magnitude of the impulsive wave. An experiment was performed using a simple shock tube with an open end and numerical calculations were carried out to solve the unsteady, axisymmetric, inviscid, compressible governing equations. The control strategy applied was to alter the exit geometry of a straight tube to a sudden enlargement tube and a flare tube. The effects of the configurations of the tube exit on the magnitude of the impulsive wave were investigated over the range of the weak shock Mach number from 1.01 to 1.10. The results obtained were compared to those of the straight tube tests. The numerical result predicted the magnitude of the experimented impulsive waves with a good accuracy. The present passive control technique enabled the magnitude of the impulsive wave to augment by about 23 percent, compared to that of the straight tube of no control.

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A Study of the Gasdynamics of Perforated Wall (다공벽의 기체역학에 관한 연구)

  • Gwak, Jong-Ho;Kim, Heuy-Dong
    • Proceedings of the KSME Conference
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    • 2003.11a
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    • pp.538-543
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    • 2003
  • Perforated wall has long been employed to control a variety of flow phenomena. It has been, in general, characterized by a porosity of the perforated wall. However, this porosity value does not take account of the number and detailed shape of porous holes, but is defined by only the ratio of the perforated area to total wall surface area. In order to quantify the porous wall effects on the flow control performance, an effective porosity should be known with the detailed flow properties inside the porous holes. In the present study, a theoretical analysis using a small disturbance method is performed to investigate detailed flow information through porous hole and a computational work is also carried out using the two-dimensional, compressible Navier-Stokes equations. Both the results are compared with existing experimental data. The gasdynamical porosity is defined to elucidate the effect of perforated wall.

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Reduction of the Cavity Flow Oscillations at Supersonic Speeds (초음속 공동유동에서의 진동감소)

  • Kang, Min-Sung;Shin, Choon-Sik;Kwon, Joon-Kyung;Kim, Heuy-Dong
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2008.11a
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    • pp.345-348
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    • 2008
  • The subcavity passive control technique is used in present study. Cavity-induced pressure oscillation has been investigated numerically for a supersonic three-dimensional flow over rectangular cavities at Mach number 1.83 at the cavity entrance. The three-dimensional, compressible Navier-stokes equations are numerically solved based on a fully implicit finite volume scheme. The results showed that the resultant amount of attenuation of cavity-induced pressure oscillations was dependent on the length and thickness of the flat plate.

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Variation of the Characteristics of Shock-Interaction Flows for Different Slot-Directions (슬롯방향 변화에 따른 충격파 간섭유동 특성변화에 관한 연구)

  • Chang Sung-Ha;Lee Yong-Hee;Lee Yeol
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2006.05a
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    • pp.306-309
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    • 2006
  • Passive control of the shock wave/turbulent boundary-layer interaction control utilizing slotted plates over a cavity has been carried out. Effect of various slot configurations on the characteristics of the interactions are tested. Pitot/wall surface pressure distributions and flow visualizations including Schlierens and interference fringe patterns over a thin oil-film have been obtained at the downstream of the shock interactions. It was found that the interaction control by a certain slot-configuration could lead a reduction of the total pressure loss through the shock wave, however, the boundary layer thickness became thicker as compared with the case of no control.

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Large Capacity Passive Flow Control Vortex Valve (대용량 피동형 유량제어 와류 밸브)

  • Choi, N. H.;Chu, I.-C.;Chung, C. H.;Cho, B. H.;Song, C.-H.
    • 유체기계공업학회:학술대회논문집
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    • 2004.12a
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    • pp.635-640
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    • 2004
  • The present paper provides the design specifications and working principle of flow controlling vortex valve which will be adopted in a Korean next generation reactor (APR1400). The vortex valve is installed inside the pressurized safety injection tank of APR1400, and it passively controls the water discharge flowrate from the tank. In the present study, the performance of the vortex valve have been evaluated throughout the repeated experiments in the full-scale test facility called VAPER(VAlve Performance Evaluation Rig). Based on the experimental results, it is confirmed that the currently developed vortex valve satisfies the major performance requirements of APR1400 plant design in view of the peak discharge flowrate, pressure loss coefficient, and total discharge duration time. To achieve the highest quality of the experimental results, a quality assurance program for vortex valve tests has been strictly applied.

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Vortex Valve의 설계인자 및 성능특성 분석

  • 김영인;황영동;장문희
    • Proceedings of the Korean Nuclear Society Conference
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    • 1995.10a
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    • pp.487-494
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    • 1995
  • 원자력발전소의 안전성 향상을 목적으로 신형원자로 안전주입계통의 축압기 설계에 적용이 고려되고 있는 피동적 유량조절 장치인 vortex 밸브의 유동장을 해석하여 밸브의 특성에 영향을 미치는 주요 인자들을 도출하고 이 인자들의 영향을 분석하였다. 분석 결과 Vortex 밸브의 성능 특성은 수송유량, 제어유량, chamber의 반경, 입구면적, 마찰계수 등의 영향을 받는 것으로 나타났으며 이들 인자 중 chamber의 반경의 영향이 가장 크고 Reynolds수의 영향은 비교적 작은 것으로 파악되었다. 또한 주어진 유동조건에서 제어유량이 작은 경우 점성손실이 vortex 밸브의 유동특성에 미치는 영향이 증대되는 경향을 보였으며 유량이 증가할수록 Reynolds수의 영향은 감소하는 것으로 나타났다.

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Control of Plume Interference Effects on a Missile Body Using a Porous Extension (다공확장벽을 이용한 미사일 동체에 대한 플룸간섭 현상의 제어)

  • Young-Ki Lee;Heuy-Dong Kim
    • Journal of the Korean Society of Propulsion Engineers
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    • v.7 no.4
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    • pp.33-38
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    • 2003
  • The Physics of the Plume-induced shock and separation Particularly at a high Plume to exit pressure ratio and supersonic speeds up to Mach 3.0 with and without a passive control method, porous extension, were studied using computational techniques. Mass-averaged Navier-Stokes equations with the RNG $\kappa$-$\varepsilon$ turbulence model were solved using a fully implicit finite volume scheme and a 4-stage Runge-Kutta method. The control methodology for plume-afterbody interactions is to use a perforated wall attached at either the nozzle exit or the edge of the missile base. The Effect of porous wall length on plume interference is also investigated The computational results show the main effect of the porous extension on plume-afterbody interactions is to restrain the plume from strongly underexpanding during a change in flight conditions. With control, a change in porous extension length has no significant effect rut plume interference.

Experimental study on reduction of impulsive noise generating at exit of high-speed railway tunnel (고속철도 터널출구에서 발생하는 충격성 소음의 저감을 위한 실험적 연구)

  • Kim, Hui-Dong;Setoguchi, Toshiaki
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.20 no.7
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    • pp.2375-2385
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    • 1996
  • As a compression wave is emitted from a duct, an impulsive wave generates and causes an impulsive noise that is at present a serious environmental noise pollution. In order to clarify the acoustic characteristics of the noise and to reduce their pressure levels, a series of model experiments were conducted on the impulsive waves emitted from an open end of a shock tube. The impulsive waves with various intensities were obtained by controlling the operation pressure ratio of the shock tube. Various kinds of silencers such as the exit boxes with baffle plates, were applied to the duct exit to reduce the impulsive noises. The effects of geometry of silencers and shock Mach number on the noise reduction were clarified. From the measurements of sound pressure level, it was found that installing the baffle plate into the exit box is effective in lowering the noise level at far fields, and that the recommendable geometries of silencer are L/D=1, H/D=1 and H/D=0.75.