• 대한기계학회논문집B
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• 제20권6호
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• pp.1994-2004
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• 1996

Numerical calculation was applied to supersonic under-expanded jets, and compared with the results of a linear theory and other experiments. TVD difference scheme was employed to solve 2-dimensional and axisymmetric inviscid Euler equation. This paper aims to explore the effects of angle of divergence and design Mach number of nozzle on the structure of under-expanded jets. The angle of divergence was varied from 0 to 20 deg. The results show that the length of the first cell of the under-expanded jets decreases and Mach disk generates at lower nozzle pressure ratio, if the angle of divergence or design Mach number of nozzle increases. The distance from the nozzle exit to Mach disk in 2-dimensional jets becomes much larger than that of axisymmetric jets, and the widths of the jet boundary and the barrel shock wave are also larger than that of axisymmetric jets. Calculation results indicate that the configuration of the under-expanded jets is strongly dependent on the nozzle pressure ratio.

• 한국추진공학회지
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• 제4권4호
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• pp.70-77
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• 2000

초음속 2단벨노즐(SDBN)은 종래의 축소확대형 초음속 노즐의 벽면에 변곡점을 설치하여, 비행체의 고도에 따른 노즐내부의 유동특성을 조절하기 위한 새로운 개념의 추진노즐이다. 본 연구에서는 이러한 SDBN의 유용성과 유동특성을 조사하기 위하여 축대칭 Navier-Stokes 방정식을 유한체적법으로 수치계산하였다. 본 연구의 결과로부터 SDBN의 Base 노즐의 길이는 SDBN 내부에서 발생하는 충격파 시스템에 영향을 미칠 뿐만 아니라, 노즐 유동의 박리위치가 변곡점에 고착되는 넓은 범위의 압력비가 존재한다는 것을 알았다. 또 SDBN의 최대추력은 노즐출구에서 유동이 적정팽창 상태일 때 발생한다는 것을 알았다.

• 한국항공우주학회지
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• 제35권4호
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• pp.281-286
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• 2007

노즐 목과 출구의 면적비가 1.8인 소형 2차원 초음속 노즐에 대해서 Navier-Stokes 방정식을 수치계산으로 풀었다. 압력비와 노즐 확대부 길이를 변화시킨 경우에 대해서 해석하여 노즐 안과 출구 근처에서 충격파 구조를 살펴보았고 특히 노즐 목 근처에서 발생하는 불규칙한 압력 분포의 특성을 노즐 목 근처의 기하학적 모양에 근거해서 규명하였다. 각각 독립적으로 표준형 노즐에서 압력비를 변화시킨 경우와 압력비를 고정하고 확대부의 노즐 길이를 변화시킨 경우 사이에 서로 유사한 충격파 구조 변화가 관찰되었고 여기에서 한 개의 경사 충격파로 오인될 수 있는 서로 다른 경사 충격파에 의해 만들어지는 수직 충격파도 포착하였다.

• Journal of Advanced Marine Engineering and Technology
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• 제32권8호
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• pp.1231-1239
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• 2008

The characteristics of flow on unventilated dual jets was experimentally investigated. The two nozzles each with an aspect ratio of 20 were separated by 6 nozzle widths. Reynolds number based on nozzle width was set to 5,000 by nozzle exit velocity. All measurements were made over a range of nozzle-to-nozzle angles from $0^{\circ}$ to $25^{\circ}$. The particle image velocimetry and pressure transducer were employed to measure turbulent velocity components and mean static pressure, respectively. It was shown that a recirculation zone with sub-atmospheric static pressure was bounded by the inner shear layers of the individual jets and the nozzles plated. As nozzle-to-nozzle inclined angles were decreased, it was found that the spanwise turbulent intensity is greater than the streamwise turbulent intensity in the merging region. In the combined region, the velocity of dual jets agree well with that of single jet, but the turbulence intensity of dual jets not agree with that of single jet.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2006년도 제27회 추계학술대회논문집
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• pp.323-326
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• 2006

This paper presents the computational results for the two-dimensional compressible non-reacted flow in a converging-diverging micro thrust nozzle of which the ratio of exit to throat width (0.541 in.) is 1.8. The RNG model is applied to calculate the turbulence by loading the standard coefficients. The results agreed very well with the experiments in the view of the shock structure and the pressure distribution at the various pressure ratios between the stagnation and the environmental states. The plume structures are also discussed on the view of the shock-cell structure.

• 대한기계학회논문집
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• 제10권5호
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• pp.635-644
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• 1986

A Compuressible turbulent boundary layer effect of the high temperature, accelerating gas flow through the De-Laval nozzle on combustion chamber pressure is numerically investigated. For this purpose, the coupled momentum integral equation and energy integral equation are solved by the Bartz method, and 1/7 power law for both the turbulent boundary layer velocity distribution and temperature distribution is assumed. As far as the boundary layer thicknesses are concerned, we can obtain reasonable solutions even if relatively simple approximations to the skin friction coefficient and stanton number have been used. The effects of nozzle wall cooling and/or mass flow rate on the boundary layer thicknesses and the combustion chamber pressure are studied. Specifically, negative displacement thickness is appeared as the ratio of the nozzle wall temperature to the stagnation temperature of the free stream decreases, and, consequently, it makes the combustion chamber pressure low.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집A
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• pp.752-757
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• 2001

To reduce stress concentration around the intersection between a spherical pressure vessel and a cylindrical nozzle under various load conditions using less material, the optimization for the distribution of reinforcement has researched. The ranked bidirectional evolutionary structural optimization(R-BESO) method is developed recently, which adds elements based on a rank, and the performance indicator which can estimate a fully stressed model. The R-BESO method can obtain the optimum design using less iteration number than iteration number of the BESO. In this paper, the optimized intersection shape is sought using R-BESO method for a flush and a protruding nozzle. The considered load cases are a radial compression, torque and shear force.

• 한국군사과학기술학회지
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• 제4권2호
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• pp.256-262
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• 2001

Viscous solutions of supersonic side jet nozzle and supersonic jet impinging on a flat plate are simulated using three-dimensional Navier-Stokes solver. For rapid and abrupt control of a missile in supersonic flight, side jet on a missile body is found to be a useful devise as evidenced by recent missile development at several nations. The magnitude of the side jet and the duration of it decide the level of control of such a missile system. The aerodynamic characteristics of the side jet devise itself are examined in terms of key parameters such as the side jet nozzle geometry, the chamber pressure and temperature. On the other hand, the jet impinging flow structure exhibits such complex nature as shock shell, plate shock and Mach disk depending on the flow parameters. Among others, the dominant parameters are the ratio of the nozzle exit pressure to the ambient pressure and the distance between the nozzle exit plane and the impinging plane. As the plate is placed close to the nozzle, the computed wall pressure at or near the jet center oscillates with large amplitude with respect to the mean value. The amplitude of wall pressure fluctuations subsides as the plate/nozzle distance increases, and the frequency of the wall pressure is estimated on the order of 10.0 KHz. Objectives of this paper are to show accurate simulation of nozzle flow itself and to demonstrate the jet flow structure when the jet interacts with a wall at a close range.

• 에너지공학
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• 제22권4호
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• pp.413-419
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• 2013

본 연구에서는 동심원관 형태의 MILD 연소로에서 바깥 원통의 배기가스 통로에서부터 안쪽 원통의 연소통로 사이에 연결관을 설치하고 배기가스를 유입하기 위해 벤츄리 노즐을 사용할 경우 벤츄리 노즐의 기하학적 형상 변화와 고압공기 노즐의 유속 변화에 따라 고압공기 유량, 배기가스 유입량 특성을 수치해석을 통해 살펴봄으로써 최적의 벤츄리 노즐 형상과 고압공기 유속 조건들을 도출하는 것을 본 연구의 목적으로 하였다. 본 연구의 전산 해석을 통해 고압공기 노즐 출구가 연소로 벽면에 부착된 경우와 배기가스에 노출된 경우를 비교하였고, 이 두 가지 형상에 대하여 고압공기 노즐과 벤츄리 노즐의 간격을 고압공기 노즐 직경의 1배에서 3배로 변화할 때의 유입량 특성을 살펴보았다. 또한 고압공기 노즐에서의 출구 유속을 변화하여 유입량 특성을 살펴보았다. 이를 통해 고압공기 노즐과 벤츄리 노즐의 간격이 증가하면 고압공기 노즐이 벽면에 부착된 경우는 유입량이 상대적으로 변화가 적으나 배기가스에 노출된 경우는 유입량이 증가하는 경향을 확인하였다. 또한 고압공기 노즐의 유속이 증가하면 속도가 낮은 범위에서는 유입량비가 상대적으로 증가하는 경향이 크지만 속도가 큰 영역에서는 증가하는 경향이 줄어드는 것을 확인하였다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 추계학술대회논문집B
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• pp.417-422
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• 2001

The shock structure of supersonic, dual, coaxial jet is experimentally investigated. Eight different kinds of coaxial, dual nozzles are employed to observe the major features of the near field shock structure of the supersonic, coaxial, dual jets. Four convergent-divergent supersonic nozzles having the Mach number of 2.0 and 3.0, and are used to compare the coaxial jet flows discharging from two sonic nozzles. The primary pressure ratio is changed in the range between 4.0 and 10.0 and the assistant jet pressure ratio from 1.0 to 4.0. The results obtained show that the impinging angle, nozzle geometry and pressure ratio significantly affect the near field shock structure, Mach disk location and Mach disk diameter. The annular shock system is found depending the assistant and primary jet pressure ratios.