• 상하수도학회지
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• 제21권3호
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• pp.287-294
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• 2007

When we use the circular pipes for wastewater and storm water, we should be known the characteristics of the flow for accurate design. To elevate the design accuracy, we want to know the profile of flow. The roughness coefficient in the Manning equation is constant, but in actuality changed with the relative depth in circular pipe. This study was conducted to calculate the relative normal depth in changing the roughness coefficient (named relative roughness coefficient) with the relative depth in the analysis of gradually varied flow in the circular pipe by Newton-Raphson method. We performed the analysis of gradually varied flow using the relative normal depth and the relative roughness coefficient. We presented the 12 flow profiles with the relative depth and the relative roughness coefficient in circular pipe. The flow classification considering relative depth in circular pipe is available to analyse gradually varied flow profiles.

• 한국수자원학회논문집
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• 제41권12호
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• pp.1173-1185
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• 2008

노면배수시설의 설계방법을 임계지속시간의 고려 여부와 등류 및 부등류의 해석 방법에 따라 4가지로 구분하고, 각 방법에 따른 설계결과를 비교·검토하였다. 임계지속시간을 고려하지 않는 방법에서 설계강우는 10분 지속시간의 강우강도로 정하나, 임계지속시간을 고려할 경우 설계강우는 강우의 지속시간과 유출의 도달시간이 유사해지는 경우를 시산적으로 찾아 결정한다. 4가지 설계방법으로 수립된 설계모형을 다양한 수로의 종단경사 및 길어깨 횡단경사를 가지는 노면배수시설에 적용하고, 그 설계결과를 비교 검토하였다. 10분 지속시간의 강우강도를 이용하는 경우, 부등류 해석을 기반으로 설계한 유출구 간격은 종단경사와 길어깨 횡단경사가 작은 경우에만 등류 해석보다 크게 산정되었다. 반면 도달시간을 산정하여 임계지속시간을 결정하는 경우에는 본 연구에서 고려된 모든 조건에서 부등류 해석을 기반으로 설계한 유출구 간격이 등류 해석보다 크게 산정되었다. 그러나 도달시간을 산정하여 임계지속시간을 결정하고 부등류 해석을 기반으로 설계한 유출구 간격은 10분 지속시간의 강우강도를 적용하고 등류 해석을 기반으로 설계한 값보다 항상 작은 것으로 조사되었다.

• 한국분무공학회지
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• 제9권2호
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• pp.24-33
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• 2004

The effect of the working fluid flow conditions and nozzle geometry on the spray performance of a twin-fluid nozzle used in Selective Catalytic Reduction is investigated experimentally. The liquid pressure is varied in the range of 0.3atm to 1.5atm and the air pressure is varied from the 0.5atm to 3.0atm. relative position between liquid nozzle(internal nozzle) and air nozzle(external nozzle) tip changes front 1mm inside the air nozzle to 1mm outside the air nozzle. The orifice diameter of the air nozzle is varied with 5mm. 6mm and 7mm. Spray visualization is realized with CCD-Camera. SMD(Sauter Mean Diameter) and mean particle velocities are measured by PDPA(Phase Doppler Particle Analyzer) under various experimental conditions. The measuring point is 300mm away from the nozzle tip in the downstream spray. The experimental results are that spray angle is depended air flow rate because nozzle diameter, air pressure and nozzle tip relative positions are related air flow rate. SMD is depended air flow rate and water flow rate. Also, SMD is increased when water flow rate is bigger. SMD is decreased when Air flow rate is bigger.

• 한국연소학회:학술대회논문집
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• 한국연소학회 2000년도 제20회 KOSCO SYMPOSIUM 논문집
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• pp.35-44
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• 2000

It was numerically studied that NOx emission characteristics of confined $CH_{4}$ jet flames with the variation of the diameter of inner fuel nozzle, the flow rate of $CH_{4}$ and equivalence ratio. Parabolic type equations were adopted in the calculation and GRI-2.1I mechanism was used for the chemical reaction. NOx emission index (EINOx) was introduced to evaluate NOx emission quantitatively in parametrically varied flames and the contribution of Thermal and Prompt NO mechanism was discussed. The results showed that Total EINOx varied sensitively with the variation of the flow rate of$CH_{4}$ but it was not sensitive to the variation of the diameter of inner fuel nozzle. Thermal EINOx showed the similar tendency to total EINOx and Prompt EINOx showed insensitivity to the variation of the diameter of inner fuel nozzle and the flow rate of $CH_{4}$.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2003년도 추계학술대회
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• pp.496-501
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• 2003

Computational study is performed to understand the fluidic thrust vectoring control of an axisymmetric nozzle, in which secondary gas injection is made in the divergent section of the nozzle. The nozzle has a design Mach number of 2.0, and the operation pressure ratio is varied to obtain the different flow features in the nozzle flow. The injection flow rate is varied by means of the injection port pressure. Test conditions are in the range of the nozzle pressure ratio from 3.0 to 8.26 and the injection pressure ratio from 0 to 1.0. The present computational results show that, for a given nozzle pressure ratio, an increase of the injection pressure ratio produces increased thrust vector angle, but decreases the thrust efficiency.

• 한국안전학회지
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• 제25권6호
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• pp.22-27
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• 2010

Flow Coefficients of intake port in an engine cylinder head were measured by a newly designed flow rig. In measuring the flow coefficient with traditional method, the valve lift was manually varied by technician with adjusting a micrometer which is directly connected to the intake valve of the cylinder head. The cam shaft of the cylinder head is directly rotated by a step motor and the valve lift was automatically varied with cam shaft profile in the newly designed flow rig. The measurement of the flow coefficient was automated by rotating the cam shaft with the step motor. Automatic measurement of the flow coefficient could be safely measured by separating a technician from the noise and vibration of the traditional flow rig. Also, the automatic measurement of the flow coefficient reduce the measurement time and provide meaningful statistical data.

• Korean Journal of Hydrosciences
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• 제5권
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• pp.1-16
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• 1994

In this paper distributed models for simulating spatially and temporally varied moving storm in a watershed were developed. The complete simulation in a watershed is achieved through two sequential flow simulations which are overland flow simulation and channel network flow simulation. Two dimensional continuity equation and momentum equation of kinematic approximation were used in the overland flow simulation. On the other hand, in the channel network simulation two types of governing equations which are one dimensional continuity and momentum equations between two adjacent sections in a channel, and continuity and energy equations at a channel junction were applied. The finite difference formulations were used in the channel network model. Macks Creek Experimental Watershed in Idaho, USA was selected as a target watershed and the moving storm on August 23, 1965, which continued from 3:30 P.M. to 5:30 P.M., was utilized. The rainfall intensity fo the moving storm in the watershed was temporally varied and the storm was continuously moved from one place to the other place in a watershed. Furthermore, runoff parameters, which are soil types, vegetation coverages, overland plane slopes, channel bed slopes and so on, are spatially varied. The good agreement between the hydrograph simulated using distributed models and the hydrograph observed by ARS are Shown. Also, the conservations of mass between upstreams and downstreams at channel junctions are well indicated and the wpatial and temporal vaiability in a watershed is well simulated using suggested distributed models.

• Ecology and Resilient Infrastructure
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• 제8권4호
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• pp.223-232
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• 2021

일반적으로 도심지에서의 유출은 도로 노면을 따라 유출되어 빗물받이를 통해 우수관거로 배수된다. 따라서 적절한 도로 배수능력의 평가는 도로와 빗물받이 뿐만 아니라 우수관거의 설계에서도 필수적이다. 하지만 도시 도로부의 지형학적 및 수리학적 조건을 반영한 흐름해석 방안에 대한 명확한 기준이 제시되어 있지 못한 실정이다. 그러므로 기존에 적용되던 흐름해석 모형(등류/ 부등류) 및 도달시간 산정방법 (임계/고정)을 분석하여 최적의 도로의 흐름해석 방안이 제시되어야 한다. 본 연구에서는 도로 표면 흐름해석을 위한 알고리즘을 개발하고 등류와 부등류 흐름해석 모형 및 도달시간 산정방법을 매개변수로 적용한 수치적 분석을 수행하여 다양한 도로조건에서의 강우 유출특성을 모의하였다. 도로조건은 국내의 설계기준을 고려하여 2차선 도로의 폭 (6 m)과 경사 (도로 종경사 1 - 10%, 도로 노면경사 2% 및 측구 횡경사 2 - 10%)가 고려되었다. 또한, 도로 표면의 흐름은 노면경사를 따라 측구에서 차집되어 하류부의 빗물받이를 통해 배수되도록 하였으며, 측구의 폭은 0.5 m로 선정하였다. 모의 결과 도로의 유출특성은 도로 경사 조건에 따라 민감하게 변화하였으며, 부등류 해석모형이 도로의 하류부로 강우가 차집되며 변화하는 측구부에서의 유출특성을 반영하여 등류 흐름해석 모형에 비해 최대 23.66%, 평균 11.80% 긴 도달시간과 최대 9.50%, 평균 4.73% 작은 도로 표면 총 유출량을 나타냈다. 따라서, 우수 유출량을 산정하기 위하여 도달시간을 강우의 지속시간으로 반영하는 임계지속시간을 적용한 부등류 흐름해석을 수행하는 것이 적합하다고 판단되었다. 개발된 알고리즘은 다양한 흐름해석 기법을 통합하여 도로 노면에서의 유출특성을 정밀하게 모의하고 있으므로 도로의 배수 설계에 활용이 가능할 것으로 기대된다.

• 한국가시화정보학회지
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• 제14권2호
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• pp.12-17
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• 2016

In this work, we investigate the flow velocity controllability of a diffuser-type multiple hydrofoil duct by experimental and numerical flow visualization approaches. The flow velocity controllability is analyzed by changing the angle of the hydrofoil near the outlet, which is the diffuser, while the incoming flow velocity is 0.6 m/s in the experiment. When the diffuser angle is changed from 0 to 7.5 degree, the maximum velocity inside the duct is varied from 1.35 m/s to 1.52 m/s. Also, it is shown from the numerical analysis that the maximum velocity is varied from 1.09 m/s to 1.17 m/s in the same condition. Thus, the aspect of the acceleration in the duct due to the increase of the diffuser angle is similar between the both approaches. Therefore, the multiple hydrofoil duct can be used to control the flow speed inside the duct for continuously extracting power close to a rated capacity.

• 한국환경과학회지
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• 제17권9호
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• pp.957-968
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• 2008

The purpose of this study is to analyze the characteristics of hydraulic behavior of the natural channel flow according to the temporal classification mode, and thus propose the hydraulic analysis method for future channel design. For analysis, the temporal flow characteristics of the channel section was divided into the steady flow and the unsteady flow. For hydraulic analysis, the HEC-RAS model, which is a one-dimensional numerical analysis model, and the SMS-RAM2 model, which is a two-dimensional model, were used and the factors used for analysis of hydraulic characteristics were flood elevation and flow rate. The flow state was analyzed on the basis of the one-dimensional steady flow and unsteady flow for review. In the unsteady flow analysis the flow rate changed by $(-)0.16%{\sim}(+)0.26%$, and the flood elevation varied by $(-)0.35%{\sim}(+)0.51%$ as compared to the values in the steady flow analysis. Given these results, in the one-dimensional flow analysis based on the unsteady flow the flood elevation and flow rate were greater than when the analysis was done on the basis of the steady flow. The flow state was analyzed on the basis of the two-dimensional steady flow and unsteady flow. In the unsteady flow analysis the flow rate varied by $(-)0.16%{\sim}(+)1.08%$, and the flood elevation changed by $(-)0.24%{\sim}(+)0.41%$ as compared to the values in the steady flow analysis. Given these analysis results, in the two dimensional flow analysis based on the unsteady flow, the flood elevation and flow rate were greater than when the analysis was done on the basis of the steady flow.