• 제목/요약/키워드: 삼각익

검색결과 16건 처리시간 0.022초

3차원 patched-grid 알고리즘을 이용한 삼각 날개-원통형 동체 형상 전산 해석 (Computational Analysis of the Delta Wing-Cylindrical Body Configuration Using the Three-Dimensional Patched-Grid Algorithm)

  • 박현돈;김영진;박수형
    • 한국항공우주학회지
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    • 제48권2호
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    • pp.109-117
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    • 2020
  • 기존 정렬 격자의 많은 제약 조건들을 완화할 수 있는 patched-grid 알고리즘을 이용하여 효율적으로 정렬 격자계를 구성하였다. EFD-CFD 워크숍의 case 4: 삼각 날개-원통형 동체 형상에 크게 3가지의 접근 방식을 적용하여 기존의 격자 생성 문제점들을 해결하였고, 실험값과 비교하여 검증하였다. 고 받음각 영역에서 표면 압력 분포가 실험값과 다소 차이를 보였다. 마하수의 증가에 따른 피칭 모멘트의 기울기 변화를 분석하였고 이는 tuck under 현상으로 설명할 수 있었다. 초음속 영역에서는 형상 앞에 궁형 충격파가 발생함으로써 삼각익 뒷전까지 양력을 발생시키는 영역이 확장되었다. 또한, 마하수와 받음각에 따라 압력 중심과 무게 중심의 위치를 비교하여 피칭 모멘트의 경향성을 분석하였다.

초경량 고정익무인항공기 사진측량기법의 정사영상 정확도 평가 (Orhtophoto Accuracy Assessment of Ultra-light Fixed Wing UAV Photogrammetry Techniques)

  • 이인수;이재원;김수정;홍순헌
    • 대한토목학회논문집
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    • 제33권6호
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    • pp.2593-2600
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    • 2013
  • 본 연구는 최근 국내외에서 문화재 보존, 사고현황조사, 군 정찰업무, 재난관리 등 다양한 분야에서 활용되고 있는 초경량 고정익무인항공기 사진측량의 성능평가를 다루고자 한다. 항공삼각측량 결과, 위치(X, Y)에서 RMSE 값은 약 10 cm로 나타났으며, UAV 사진측량의 정사영상에 대한 시각판독법(on-screen digitizing) 기법과 지상측량에 의한 필계점 좌표 차의 RMSE 는 X 방향 약 0.174~0.205 m, Y방향 약 0.294~0.298 m의 편위형 오차가 도출되었다. 그리고 실험대상지역의 임의의 1 필지를 대상으로 지적 공부대장면적과 UAV 사진측량의 정사영상으로 취득한 필지 면적을 비교한 결과 차이는 0.118 $m^2$이다. 본 연구는 초경량 고정익무인항공기 사진측량의 정사영상 정확도 평가에 대한 하나의 연구 사례를 제시하였으며, 향후 항공삼각측량(AT), 직접 기하보정(direct-georeferencing), 비행계획, 그리고 실용적 응용분야 개발 등에 대한 연구가 지속되어야 할 것으로 판단된다.

배연탈질설비의 성능향상을 휘한 가스혼합에 관한 연구 (A Study on the Flue Gas Mixing for the Performance Improvement of De-NOx plant)

  • 류병남
    • Journal of Advanced Marine Engineering and Technology
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    • 제23권4호
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    • pp.462-472
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    • 1999
  • De-NOx facility using Selective Catalytic Reduction method is the most widely applied one that removes NOx from flue gas emitted from combustion facility such as boiler for power generation engine incinerator etc. Reductant $NH_3\;or\;NH_4OH$ is sprayed into flue gas to convert NOx into $H_2O$ and $N_2.$ Good mixing between flue gas and $NH_3$ is the most important factor to increase reduction in catalytic layer and to reduce unreacted NH3 slip. Therefore the development of mixer device for mixing effect is one of the important part for SCR facility. Objectives of this study are to investigate the relation between flow and concentration field by observation at the wake of delta-wing type mixer. At the first stage qualitative measurement of flow field is conducted by flow visualization using laser light sheet in lab. scale wind tunnel. Also we have conducted the quantitative analysis by comparing flow field measurement using LDV with numerical simulation. On the basis of qualitative and quantitative analysis we investigate the dis-tribution of flow and concentration in flow model facility. The results of an experimental and compu-tational examination of the vortex structures shed from delta wing type vortex generator having $40^{\circ}$ angle of attack are presented, The effects of vortex structure on the gas mixing is discussed, too.

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문턱치값 최적화 연구 (A Study of the Threshold value Optimization)

  • 서정익;박은규
    • 한국정보컨버전스학회논문지
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    • 제7권2호
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    • pp.7-12
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    • 2014
  • 정확한 신호의 검출을 위해서 많은 필터들이 만들어지고 있다. 필터의 성능은 잡음을 효과적으로 제거하는 것으로 평가한다. 필터의 정확한 평가를 위해서 문턱치 값을 효과적으로 결정할 필요가 있다. 본 연구에서는 문턱치 값의 최적화에 대해 연구하였다. 신호는 삼각파와 전원잡음을 이용하였다. 샘플 개수에 따른 SNR 변화를 연구하였다. 샘플 개수가 증가함에 따라 SNR도 안정화가 되었다.

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종방향 와동과 난류경계층의 상호작용에 관한 수치해석 (Numerical Simulation on Interactions of Longitudinal Vortices in a Turbulent Boundary Layer)

  • 양장식
    • Journal of Advanced Marine Engineering and Technology
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    • 제29권6호
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    • pp.637-644
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    • 2005
  • This paper describes the numerical simulation of the interaction between longitudinal vortices ("common flow up") and a 3-D turbulent boundary layer over a flat plate To analyze the common flow up Produced from vortex generators. the flow field behind the vortex generators Is modeled by the information that is available from studies on a half-delta winglet. Also. the Reynolds-averaged Navier-Stokes equation for three-dimensional turbulent flows. together with a two-layer turbulence model to resolve the near-wall flow, is solved by the method of AF-ADI. The computational results predict that the boundary layer is thinned in the regions where the secondary flow is directed toward the wall and thickened where it is directed away from the wall Also. the numerical results. such as Reynolds stresses. turbulent kinetic energy and skin friction characteristics generated from the vortex generators . are reasonably close to the experimental data.

3차원 난류경계층 내에 존재하는 종방향 와동의 유동장 및 열전달 특성에 관한 수치해석(II) - Common Flow Up에 관하여 - (Numerical Analysis on the Flow Field and Heat Transfer Characteristics of Longitudinal Vortices in Turbulent Boundary Layer - On the Common Flow Up -)

  • 양장식
    • 설비공학논문집
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    • 제17권9호
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    • pp.799-807
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    • 2005
  • The flow characteristics and the heat transfer rate on a surface by the interaction of a pair of vortices are studied numerically. To analyze the common flow up produced by vortex generators in a rectangular channel flow, the pseudo-compressibility viscous method is introduced into the Reynolds-averaged Navier-Stokes equation for 3-dimensional unsteady, incompressible viscous flows. To predict turbulence characteristics, a two-layer $k-\varepsilon$ turbulence model is used on the flat plate 3-dimensional turbulence boundary The computational results predict accurately Reynolds stress, turbulent kinetic energy and flow field generated by the vortex generators. The numerical results, such as thermal boundary layers, skin friction characteristics and heat transfers, are also reasonably close to the experimental data.

사각채널내 와동발생기가 부착된 원형실린더 하류 유동 특성에 대한 실험적 연구 (Experimental Investigations of Flow Characteristics by Wing Type Vortex Generators Set up Behind a Circular Cylinder in a Rectangular Channel)

  • 이상민;하홍영;양장식;이기백
    • Journal of Advanced Marine Engineering and Technology
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    • 제25권5호
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    • pp.1076-1085
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    • 2001
  • Experimental investigations of the longitudinal vortices, which are produced by wing type vortex generators set up behind a circular cylinder in a rectangular channel, are presented. When the circular cylinder is set up in the rectangular channel, a horseshoe vortex is formed just upsteam of the circular cylinder. It generates a turbulent wake region behind the circular cylinder. Therefore, the region of the pressure loss behind the circular cylinder in increased and the size of the wake is small. These problems can be achieved by longitudinal vortices which are generated by wing-type vortex generator. In order to control the strength of longitudinal vortices, the angle of attack of the vortex generators is varied from 20 degree to 45, but the spacing between the vortex generators is fixed 6cm. The 3-dimensional mean velocity measurements are made using a five-hole probe. The vorticity field and streamwise velocity contour are obtained from the velocity field. The following results are obtained. Circulation strength is the maximum value when the angle of attack($\beta$) is $30^{\circ}$, and the vorticity field and streamwise velocity contour in case of $\beta$=$20^{\circ}$ show the trend similar to these in case of $\beta$=$30^{\circ}$, but do not in case of $\beta$=$45^{\circ}$.

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종방향 와동이 유체유동 및 열전달 특성에 미치는 영향에 관한 실험적 연구 (An Experimental Study on the Effect of Fluid Flow and Heat Transfer Characteristics by the Longitudinal Vortices)

  • 양장식;김은필
    • 설비공학논문집
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    • 제12권9호
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    • pp.843-852
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    • 2000
  • The flow characteristics and the heat transfer rate on a surface by interaction of a pair of vortices were studied experimentally. The test facility consisted of a boundary-layer wind tunnel with a vortex introduced into the flow by half-delta winglet protruding from the surface. In order to control the strength of the longitudinal vortices, the angles of attack of the vortex generators were varied from $\pm20\;degree\;to\;\pm45$ degree, but spacings between the vortex generators were fixed to 4 cm. The 3-dimensional mean velocity measurements were made using a five-hole pressure probe. Heat transfer measurements were made using the thermochromatic liquid to provide the local distribution of the heat transfer coefficient. By using the method mentioned above, the following conclusions were obtained from the present experiment. The boundary layer was thinned in the regions where the secondary flow was directed toward the wall and thickened where it was directed away from the wall. The peak augmentation of the local heat transfer coefficient occurred in the downwash region near the point of minimum boundary-layer thickness.

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원주 후미에 부착된 와동발생기의 영각 변화에 따른 유동 및 열전달 특성 (Flow and Heat Transfer Characteristics due to the Variations of the Angle of Attack at the Vortex Generators located behind a Circular Cylinder)

  • 하홍영;홍철현;양장식;이기백
    • Journal of Advanced Marine Engineering and Technology
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    • 제26권4호
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    • pp.439-449
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    • 2002
  • Experimental investigations of the flow structure and heat transfer enhancement in a channel with a built-in circular cylinder and a wing-let type vortex generator are presented. Without any vortex generators, relatively low heat transfer takes place in the downstream of the circular cylinder where is a recirculation region with low velocity fluid is formed. However with a wing-let type longitudinal vortex generator in the wake region behind the cylinder, heat transfer in the region can be enhanced. In order to control the strength of longitudinal vortices, the angle of attack of the vortex generators is varied from $20^{circ} to 45^{\circ}$, but spacings between the vortex generations are fixed to be 5 mm. The 3-dimensional mean velocity field downstream of the vortex generator is measured by a five-hole pressure probe, and the hue-capturing method using thermochromatic liquid crystals has been used to provide the local distribution of the heat transfer coefficient. The vorticity field and streamwise velocity contour are obtained from the velocity field. Streamwise distributions of averaged Stanton number on the measurement planes show very similar trends for all the experimental cases($\beta=20^{circ}, 30^{circ} and 45^{\circ}$). Circulation strength and heat transfer coefficient have the maximum values when the angle of attack($\beta$) is $30^{\circ}$.