• 대한기계학회논문집B
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• 제29권8호
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• pp.934-939
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• 2005

Starting pressure of a supersonic ejector with a second-throat was investigated. In case of mixing chamber length longer than a critical length, starting pressure is in proportion to length of the mixing chamber. In this study, we assumed that the ejector starts when the primary supersonic flow reaches inlet of the second-throat and the distance of the supersonic flow traveling can be expressed by multiplying an empirical factor to the first diamond shock length of overexpanded flow. To calculate the overexpanded supersonic flow, a mixing model was employed to compute secondary flow pressure and the result was applied to back pressure condition of overexpanded flow calculation. In the result, for three cases of primary nozzle area ratio, we could get accurate model of predicting the starting pressure by selecting a suitable empirical factors around 3.

• Journal of Mechanical Science and Technology
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• 제15권8호
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• pp.1174-1180
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• 2001

Various experimental data, including mixing areas, cross correlation factors, surface flow patterns on nozzle walls, and far field noise spectra, was used to draw a noise control mechanism in a supersonic jet. In the underexpanded case, mixing of the jet air with ambient air was significantly enhanced as presented before, and mixing noise was also dramatically reduced. Screech tones, in the overexpanded case, were effectively suppressed by trailing edge modifications, although mixing enhancement was not noticeable. From mixing and noise performance of nozzles with modified trailing edges, enhancing mixing through streamwise vortices seems an effective way to reduce mixing noise in the underexpanded flow regime. However, screech tones in the overespanded flow regime is well controlled or suppressed by making shock cells and/or spanwise large scale structures irregular and/or less organized by a proper selection of trailing edges. The noise field in the overexpanded flow regime was greatly affected by the symmetricity of the nozzle exit geometry. In the underexpanded flow regime, the effects of the symmetricity of the nozzle exit on mixing were negligible.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2004년도 제22회 춘계학술대회논문집
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• pp.408-413
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• 2004

Numerical and experimental investigation were car-ried out to clarify the flow structure of underexpanded jet from a square nozzle. The square nozzle rep-resents one of the clustered combustors of a linear aerospike engine. From the numerical results, the three-dimensional shock wave of the underexpanded square jet was found to be composed of two shocks. One is the intercepting shock which corresponds to the shock observed in two-dimensional planar jet. The other is the recompression shock divided into two types. The expansion fans coming from the nozzle edges interact with each other at the comers of the nozzle exit, and overexpanded regions are generated. Therefore one of the two recompression shocks is formed at the comers of the nozzle exit behind the overexpanded regions. As the jet goes downstream, the overexpanded regions grow larger to coalesce at the symmetry planes. Then, the other type of the recompression shock is generated. The three-dimensional shock structure formed by the intercepting shock and the recompression shocks dominates the expansion of the jet boundary. The shock detection algorithm us-ing CFD results was developed to reveal the relation between the shock waves and the jet boundary, and it was found that the cross-sectional jet shape becomes cross-shape. The key features observed in the numerical investigation were verified by the experimental results. The shock structure at the diagonal plane was in good agreement with the experimental schlieren images. Moreover, the cross-sections visualized by the Mie scattering method confirmed that the cross-section of the jet becomes cross-shape.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2005년도 창립60주년 기념 추계 학술대회
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• pp.75.2-75.2
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• 2005

• 한국추진공학회지
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• 제18권4호
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• pp.1-8
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• 2014

과대팽창이 발생하는 축대칭 초음속 노즐에서 노즐압력비가 충격파 구조와 추력성능에 미치는 영향을 규명하기 위해 지상연소시험평가용 추력기 노즐을 대상으로 수치모사를 수행하였다. k-${\omega}$ SST 난류 모델을 적용한 Reynolds-averaged Navier-Stokes 방정식을 상용코드 FLUENT를 사용하여 해석한 결과, 노즐 압력비가 증가함에 따라 추력성능이 단조적으로 증대되고, 노즐 내부에서 생성된 충격파와 유동박리점이 노즐 출구방향으로 밀려나는 사실을 확인하였다. 또, 노즐내부 충격파와 팽창파 위치의 직접적 영향을 받는 노즐 출구면에서의 유동구조가 추력성능에 미치는 영향도 상세히 조사하였다.

• 한국추진공학회지
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• 제6권2호
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• pp.1-7
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• 2002

추진기관은 노즐을 통해 추력을 발생하며 축소-확대 형상의 초음속 노즐에서는 노즐의 설계 팽창비가 내부 유동의 전압력과 배압의 압력비보다 매우 클 때 충격파의 발생과 함께 경계층 박리를 유발한다. 노즐 내부에서의 충격파 발생과 유동의 박리는 주어진 유동의 압력비에 가장 적합한 노즐형상을 구현하는 것으로 실제의 구조적 노즐의 형상보다 짧은 노즐에서 나타나는 유동과 같은 현상을 보인다. 수치 해석적 방법으로 고정된 형상의 2차원 노즐 내부의 충격파와 경계층 박리 현상에 관한 연구를 수행하였고 Hunter가 행한 실험적 연구와 비교하였다. 수치해석은 TVD 기법을 이용한 압축성 유체 해석 코드와 SST 2방정식 난류 모델을 이용하여 수행되었다. 낮은 압력비에서의 충격파와 경계층과의 상호작용에 의한 $\lambda$형태의 충격파 시스템을 잘 보여주고 있고 추력 값의 비교를 통해 고정된 형상의 노즐을 이용하여 필요한 운용범위를 충족할 수 있음을 알 수 있었다.

• Advances in aircraft and spacecraft science
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• 제7권5호
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• pp.387-404
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• 2020

The numerical simulation of shock waves in supersonic flows is challenging because of several instabilities which can affect the solution. Among them, the carbuncle phenomenon can introduce nonphysical perturbations in captured shock waves. In the present work, a hybrid numerical flux is proposed for the evaluation of the convective fluxes that avoids carbuncle and keeps high-accuracy on shocks and boundary layers. In particular, the proposed flux is a combination between an upwind approximate Riemann problem solver and the Local Lax-Friedrichs scheme. A simple strategy to mix the two fluxes is proposed and tested in the framework of a discontinuous Galerkin discretisation. The approach is investigated on the subsonic flow in a channel, on the supersonic flow around a cylinder, on the supersonic flow on a flat plate and on the flow in a overexpanded rocket nozzle.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2009년도 제33회 추계학술대회논문집
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• pp.253-256
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• 2009

과팽창 상태 추력 노즐 내부의 측력(Lateral Force)발생에 대한 기초적 연구 분석을 실험적, 수치 해석적 방법으로 수행하였다. 엔진 정지 과정시 추력 노즐 내에 발생하는 압력진동을 조사하였다. 구동 압력비 변화에 따른 벽 압력 분포를 측정 및 쉴리렌 가시화를 수행하였다. RSS(Restricted Shock Separation)에서 FSS(Free Shock Separation)로 천이하는 순간 벽 압력 피크값이 발생하였다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 추계학술대회논문집B
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• pp.622-627
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• 2001

Microjet flows are often encountered in many industrial applications of micro-electro-mechanical systems as well as in medical engineering fields such as a transdermal drug delivery system for needle-free injection of drugs into the skin. The Reynolds numbers of such microjets are usually several orders of magnitude below those of larger-scale jets. The supersonic microjet physics with these low Reynolds numbers are not yet understood to date. Computational modeling and simulation can provide an effective predictive capability for the major features of the supersonic microjets. In the present study, computations using the axisymmetic, compressible, Navier-Stokes equations are applied to understand the supersonic microjet flow physics. The pressure ratio of the microjets is changed to obtain both the under- and over-expanded flows at the exit of the micronozzle. Sonic and supersonic microjets are simulated and compared with some experimental results available. Based on computational results, two microjets are discussed in terms of total pressure, jet decay and supersonic core length.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 1995년도 제5회 학술강연회논문집
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• pp.69-83
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• 1995

A great number of experimental data indicating shock-induced separation(SIS) in internal or external supersonic flows were reviewed to make clear the mechanism of SIS and to present the criterion of turbulent boundary layer separation. The interesting conclusions were obtained for the considerably wide range of flow geometries that the incipient separation is almost independent of the flow geometries, and that it is relatively unaffected by changes in gas specific heat, and boundary layer Reynolds number, Furthermore, the pressure rise necessary to separate boundary layer in external flows was found to be applicable to SIS in overexpanded propulsion nozzles. This is due to the fact that the SIS phenomenon caused by the interaction between shock waves and turbulent boundary layers is processed through a supersonic deceleration. This is, the SIS in almost all of interacting flow fields is governed by the concept of free interaction, and criterion of SIS is only a Function of upstream Mach number.