• Journal of the Computational Structural Engineering Institute of Korea
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• v.30 no.1
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• pp.47-53
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• 2017

A boundary layer integral combined with a 1-D isentropic core flow model has been successfully used to determine heat transfer rate on the surface of a supersonic nozzle. However its accuracy is affected by the core flow condition which is used as a boundary condition for the integral calculation. Because flow behavior near a nozzle throat deviates from 1-D isentropic condition due to 2-D flow turning and interaction between core flow and boundary layer, accuracy of heat transfer calculation decreases at a nozzle throat. Therefore, CFD is adopted to deduce improved core flow condition and increase accuracy of boundary layer integral at nozzle throat in this research. Euler model and SST $k-{\omega}$ model is solved by CFD code and used as a boundary condition for boundary layer integral. Developed code is tested in the supersonic nozzle from the previous research and improvement in accuracy is observed, especially at nozzle throat and diverging section of the nozzle. Error between experimental result and calculation result reduced by 16% when a calculation is made based on the SST $k-{\omega}$ model. Method developed in this research is expected to be used in thermal design of the rocket nozzle.

• Proceedings of the Korea Air Pollution Research Association Conference
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• 2000.04a
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• pp.227-228
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• 2000

가상 임팩터(virtual impactor)는 가속노즐(acceleration nozzle)아래에 충돌판(impaction plate) 대신 가상의 공간을 가진 수집관(receiving tube)이 설치되어 유선의 방향이 $90^{\circ}$로 바뀔 때, 큰 입자는 유선에서 벗어나 수집노즐에 포집된다(Hounam and Sherwood, 1965). 가상 임팩터에는 관성 임팩터(inertial impactor)와는 다르게, 절단입경(cut-size)보다 큰 입자를 분리할 수 있는 부 유동(minor flow)과 절단입경보다 작은 입자를 분리할 수 있는 주 유동(major flow)으로 나눈다. (중략)

• Proceedings of the Korean Society of Propulsion Engineers Conference
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• 2000.11a
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• pp.32-32
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• 2000

3단형 과학로켓의 고체모타의 내부 유동을 추진제의 연소에 따라 내부형상이 변화하는 과정에 대해 수치해석 하였다. 추진제는 표면에서 균일하게 연소된다고 가정하였으며 연소거리가 0.1mm, 30mm, 60mm, 90mm인 경우의 고체모타 내부 물리량 변화를 관찰하였다. 연소가 진행되며 잠입형 노즐의 위 부분에 큰 재순환 영역이 생기는 것이 관찰되었으며 노즐에 작용하는 압력 힘을 구하여 본 결과 노즐부의 모멘트 힘은 크지 않은 것으로 판명되었다.(중략)

• Journal of the Korean Society for Aeronautical & Space Sciences
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• v.44 no.8
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• pp.641-648
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• 2016

In this study, the effect of injection nozzle shape on the supersonic film cooling performance is analyzed using CFD. The design parameters are inside and outside angles of upper plate of nozzle and nozzle tip thickness. It is observed that the mass flow rate of film cooling decreases with increase of inside angle, while the effect of the change of mass flow rate on the film cooling effectiveness is relatively small. In addition, cooling performance is generally reduced, except ahead of the local region where shock wave interaction with film cooling occurs, in accordance with the growth of the outside angle and tip thickness. In this paper, the CFD simulation is performed using a commercial software, ANSYS Fluent V15.0, and the CFD model is validated by comparing it with the experimental data shown in preceding research.

• Journal of the Korean Society of Propulsion Engineers
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• v.26 no.5
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• pp.11-23
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• 2022

For the design of the shortened ED(Expansion Deflection) nozzle, a numerical study of ED nozzle was performed according to the length reduction methods. The first method is to reduce the extension length of the ED nozzle with 80% bell nozzle length by 10%, 20% and 30%. The second method is to shorten the extension length by increasing the nozzle throat angle. Due to the increase in the curvature of the contour as the length shortened, the decrease in the nozzle exit velocity between the ED nozzle with 80% bell nozzle length and the ED nozzle in the first method was reduced, and the thrust become similar. The ED nozzle of the second method increased the thrust by increasing the nozzle exit velocity compared to the ED nozzle with 80% bell nozzle length.

• Proceedings of the Korean Society of Propulsion Engineers Conference
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• 1999.04a
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• pp.15-15
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• 1999

2차 유동 분사에 의한 추력 방향 제어 방법은 복잡한 기계적 작동장치와 이에 따른 무게의 증가를 배제할 수 있다. 본 연구에서는 유동 해석을 통하여 2차원 및 3차원 초음속 수축-팽창 노즐 유동에 2차 유동을 분사하여, 2차 유동의 분사 위치, 분사 유량 및 분사 각도 등이 추력의 방향 및 크기에 미치는 영향을 밝혀 추력 방향 제어를 위한 최적의 2차 분사 조건을 제시하였다. 유동 해석 결과 2차 유동의 분사 위치는 생성된 경가 충격파가 노즐 출구까지 분포되는 지점이 최대 전향각과 횡추력을 가지는 분사위치임을 알 수 있었고, 분사 각도는 주 유동의 역방향으로 분사하는 것이 수직방향으로 분사하는 것보다 더 큰 전향각을 얻을 수 있었다. 또한 2차원의 경우보다 3차원 유동에서 큰 전향각이 생김을 알 수 있었다.

• Aerospace Engineering and Technology
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• v.3 no.2
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• pp.50-55
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• 2004

Performance predictions of the propulsion system were conducted for a 900㎏ class Canard Rotor/Wing vehicle. The main components of the propulsion system are turbojet engine, exhaust ducts and nozzles. The internal flow of the duct was considered as one-dimensional, compressible and viscous flow. Adequate governing equations including centrifugal force effect were applied to the analysis of the duct flows. Results such as available power, available thrust, engine throttle, mass flow rates, rotor RPM and cruise nozzle area were presented for rotary-wing mode and transition mode.

• Proceedings of the KSME Conference
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• 2005.11a
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• pp.80.2-80.2
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• 2005

• Journal of the Korean Society of Fisheries and Ocean Technology
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• v.33 no.3
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• pp.241-247
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• 1997

터보 노즐에 유동하는 가스 에너지의 변화와 그위상의 조정에 의하여 디젤엔진의 성능 개선 가능성을 검토 하였다. 그리고 디젤기관의 각실린더와 터빈 노즐 면적과 가스의 유동에 대한 동기화를 실시함으로써 엔진 성능 또한 개선할 수 있었다.

• Journal of the Korean Society of Propulsion Engineers
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• v.4 no.1
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• pp.13-21
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• 2000

The advantages of the SITVC (Secondary Injection for Thrust Vector Control) technique over mechanical thrust vectoring systems include a reduction in both the nozzle weight and complexity due to the elimination of the mechanical actuators that are used in conventional vectoring. The optimal operating conditions of SITVC were investigated using in-house developed compressible flow analysis codes. Numerical experiments were used to examine the impact of the thrust vector direction with a variety of injection positions, mass flow rates, and injection angles on the two-dimensional expansion cone of a supersonic nozzle. The computational results showed that the optimal position of the secondary injection, with the maximum deviation angle and side thrust, was where the oblique shock generated by the secondary injection reached the end of the nozzle exit.