• 대한토목학회논문집
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• 제13권1호
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• pp.179-192
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• 1993

유한차분법으로 3차원 점성토 수송 모델 COSETM-3을 개발하여 개수로의 중층에서 시간에 따른 부유니의 상대농도에 관한 실험결과(實驗結果)와 비교하였으며, 그 결과 잘 일치하였다. 모델의 현지(現地) 적용성(適用性)과 수영만(水營灣)의 SS(Suspended Solids) 확산을 조사하기 위해 대조기(大潮期) 수평시(平水時)와 홍수시(洪水時)에 모델을 수영만에 적용하여 수영강(水營江)에서 유출되는 SS의 거동(擧動)을 해석하였으며, 그 결과 현지의 SS 거동을 정성적으로 잘 예측하였다. 침강속도가 SS의 농도분포에 미치는 영향에 대해서도 검토하였다. 침강(沈降)을 고려하지 않은 경우 SS 농도는 표층이 저층보다 높게 나타났으나, 침강(沈降)을 고려했을 경우에는 저층이 표층보다 높게 나타났다. 그리고, 표층에서는 활발한 해수교환으로 인해 SS의 변동폭이 크게 나타났으나, 저층에서는 해수교환(海水交換)이 약하기 때문에 SS의 변동폭이 상대적으로 작게 나타났다. 홍수시(洪水時) SS 확산패턴은 평수시(平水時)와 유사하게 나타났으나, SS 농도는 평수시(平水時)보다 훨씬 높게 나타났다. 첨두유량이 발생할 때까지 SS 농도는 점차 증가하였으나, 첨두유량이 발생한 이 후부터 SS 농도는 유출량(流出量)의 감소로 인해 점차 감소하였다.

• 수산해양기술연구
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• 제31권1호
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• pp.54-62
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• 1995

해상에서 어군의 행동과 분포상태를 탐지하여 그 정보를 원격으로 전송하기 위한 원격어군탐지기를 시험제작하고, 이들을 이용하여 서해의 고군산군도 연안에서 1994년 8월 8일, 18일~19일 및 9월 8~9일에 낭장망에 입망하는 어군의 유영층과 그 어획변동 등을 조사하고, 원격어군탐지기의 실용성을 평가하여 분석, 고찰한 결과는 다음과 같다. 1. 어획어종은 12종이었으며, 멸치(Engraulis japonica), 꼴뚜기(Loligo beka), 밴댕이(Harengula zunasi) 등이 전 어획량의 95%이상을 차지하였다. 2. 해상이 동국에서 탐지한 어군탐지기의 기록과 그것을 원격으로 전송한 선상고정국의 어군기록은 매우 잘 일치하였다. 3. 멸치는 유속이 0.6kt 이하로서 유속변화가 적은 경우에 어획이 많았으며, 유속이 0.6kt이상인 때에는 적어지는 경향을 나타내었다. 4. 어군의 유영층은 유속이 1kt이하에서 얕아지는 경향이 있었으며, 유속이 1kt이상이고 유속변화가 커지면 유영층에 큰 변동이 없으며, 이때 평균깊이는 약 4m였다. 5. 1회 조업당 어획량은 10~30 kg이었으며, 유향과 어구의 부설방향이 일치하지 않거나 유속이 너무 강해지면 어획이 적음을 알 수 있었다. 이상의 결과와 같이 본 연구에서 시험제작한 원격어군탐지기는 낭장망어업에서 어군의 행동과 분포에 관한 어업정보를 파악하는데 유효하게 사용할 수 있음이 확인되었다.

• 한국연소학회:학술대회논문집
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• 한국연소학회 2006년도 제33회 KOSCO SYMPOSIUM 논문집
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• pp.86-94
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• 2006

This paper investigates the effects of acoustic forcing on NOx emissions and mixing process in the near field region of turbulent hydrogen nonpremixed flames. The resonance frequency was selected to force the coaxial air jet acoustically, because the resonance frequency is effective to amplify the forcing amplitude and reduce NOx emissions. When the resonance frequency is acoustically excited, a streamwise vortex is formed in the mixing layer between the coaxial air jet and coflowing air. As the vortex develops downstream, it entrains both ambient air and combustion products into the coaxial air jet to mix well. In addition, the strong vortex pulls the flame surface toward the coaxial air jet, causing intense chemical reaction. Acoustic excitation also causes velocity fluctuations of coaxial air jet as well as fuel jet but, the maximum value of centerline fuel velocity fluctuation occurs at the different phases of $\Phi$=$180^{\circ}$ for nonreacting case and $\Phi$=$0^{\circ}$ for reacting case. Since acoustic excitation enhances the mixing rate of fuel and air, the line of the stoichiometric mixture fraction becomes narrow. Finally, acoustic forcing at the resonance frequency reduces the normalized flame length by 15 % and EINOx by 25 %, compared to the flame without acoustic excitation.

• 한국연소학회지
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• 제14권1호
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• pp.31-38
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• 2009

The effects of acoustic excitation of coaxial air on mixing enhancement and reduction of nitrogen oxides (NOx) emission were investigated. A compression driver was attached to the coaxial air supply tube to impose excitation. Measurements of NOx emission with frequency sweeping were performed to observe the trend of NOx emission according to the fuel and air flow conditions and to inquire about the effective excitation frequency for reducing NOx. Then, Schlieren photographs were taken to visualize the flow field and to study the effect of excitation. In addition, phase-locked particle image velocimetry (PIV) was performed to acquire velocity field for each case and to investigate the effect of vortices more clearly. Direct photographs and OH chemiluminescence photographs were taken to study the variation of flame length and reaction zone. It was found that acoustic forcing frequencies close to the resonance frequencies of coaxial air supply tube could reduce NOx emission. This NOx reduction was influenced by mixing enhancement due to large-scale vortices formed by fluctuation of coaxial air jet velocity.

• 대한기계학회논문집
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• 제14권2호
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• pp.298-309
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• 1990

In this paper, a new method is suggested to analyze impulsive stresses at loading poing of concentrated impact load under certain impact conditions determined by impact velocity, stiffness of plate and mass of impact body, etc. The impulsive stresses are analyzed by using the three dimensional dynamic theory of elasticity so as to analytically clarify the generation phenomenon of cone crack at the impact fracture of fragile materials (to be discussed if the second paper). The Lagrange's plate theory and Hertz's law of contact theory are used for the analysis of impact load, and the approximate equation of impact load is suggested to analyze the impulsive stresses at the impact point to decide the ranage of impact load factor. When impact load factors are over and under 0.263, approximate equations are suggested to be F(t)=Aexp(-Bt)sinCt and F(t)=Aexp(-bt) {1-exp(Ct)} respectively. Also, the inverse Laplace transformation is done by using the F.F.T.(fast fourier transform) algorithm. And in order to clarity the validity of stress analysis method, experiments on strain fluctuation at impact point are performed on a supported square glass plate. Finally, these analytical results are shown to be in close agreement with experimental results.

• 대한기계학회논문집
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• 제19권5호
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• pp.1340-1350
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• 1995

The effects of thermal stratification on the flow past a heated circular cylinder with various heating rates were examined in a wind tunnel. Turbulent intensities, r.m.s.values of temperature and turbulent convective heat flux distributions in the cylinder wakes with and without thermal stratification were measured by using a hot-wire and cold-wire combination probe. The phase averaging method was also used to estimate coherent contributions to the turbulent flow field in the near wake. The results show that the scalar mixing process is very different according to the mean temperature fields especially in the upper part of the wake. The coherent structure of the temperature field makes a large contribution to the time mean value like velocity components. However, the coherency of the temperature fluctuation is very different with the change of mean temperature fields, though the velocity coherent motions are quite similar in all experimental conditions.

• Journal of Advanced Marine Engineering and Technology
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• 제39권10호
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• pp.1017-1022
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• 2015

Specific hydrodynamic characteristic of pump-turbine during the start and load rejection process of generating mode causes anomalous increase of water pressure, along with large machine vibration, called "S" characteristic. The aim of this study is to understand and explain the hydrodynamic performance of pump-turbine at "S" characteristic region by using a model of pump-turbine system. The operation in the condition of runway and low discharge in a typical "S" characteristic curve may become unstable and complex flow appears at the passage of guide vane and impeller. Therefore, velocity and pressure distribution are investigated to give an all-sided explanation of the formation and phenomenon of this characteristic, with the assistance of velocity triangle analysis at the impeller inlet. From this study, the internal flow and pressure fluctuation at the normal, runway and low discharge points are explored, giving a deep description of hydrodynamic characteristic when the pump-turbine system operates with "S" characteristic.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2004년도 Proceedings of 2004 Korea-Japan Joint Seminar on Particle Image Velocimetry
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• pp.147-155
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• 2004

Self-excited noise generation from laminar flames in thin annular jets of methane/air premixture has been investigated experimentally. Various flames were observed in this flow configuration, including conical shape flames, ring shape flames, steady crown shape flames, and oscillating crown shape flames. Self-excited noise with the total sound pressure level of about 70dB was generated from the oscillating crown shape flames for the equivalence ratio larger than 0.95. Sound pressure and $CH^*$ chemiluminescence were measured by using a microphone and a photomultiplier tube. The frequency of generated noise was measured as functions of equivalence ratio and premixture velocity. A frequency doubling phenomena have also been observed. The flame shape during flame oscillation was reconfirmed by a synchronized PIV experiment. The velocity and pressure field were obtained from PIV. The minimum pressure was formed near the edge of flame representing circulation. By comparing the results of sound pressure, flame luminosity and PIV, the noise source can be attributed to the flame front fluctuation near the edge of the oscillating crown-shape flames.

• 대한기계학회논문집
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• 제14권5호
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• pp.1282-1289
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• 1990

본 연구에서는 원관내에서 동적으로 완전히 발달한 난류맥동유동에서 관벽에 서 균일한 열유속이 주어지는 경우에 대하여 난류모델로서 K-.epsilon. 2방정식 모델을 적용 하여 수학적인 모델을 세운 후 이를 수치적으로 해석하였다. 그 결과 시간평균 레이 놀즈수가 10000인 경우에 대하여 Strouhal수가 0.0005에서 0.05 그리고 맥동속도진폭 이 0.8이하인 맥동류에 대한 열전달 특성을 제시하였다.

• Ocean and Polar Research
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• 제21권2호
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• pp.99-108
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• 1999

With sectional data obtained in September of 1987, 1988 and 1989 by quadrireciprocal ADCP measurement and CTD cast, the current structure, volume transport and vorticity in the Western Channel of the Korea Strait were studied. The characteristics of Tsushima Current water persisted throughout the summer especially in the homogeneous water of temperature $14-16^{\circ}C$ located at the depth of 50-100m below seasonal termocline. Thickness and velocity of the homogeneous layer are about 10-170m and 20-60cm/s. and the relative vorticity for this layer is shown to be nearly constant and it is smaller than the planetary vorticity. Potential vorticity of $2.70-7.10{\times}10^{-6}m^{-1}s^{-1}$ is found to be dependent mainly on planetary rather than on the relative vorticities. The Tsushima Current water represented by the homogeneous layer R14-16^{\circ}C$ may keep the potential vorticity at the area of strong current in the Strait. The ADCP current structure is similar to geostrophic current and the core of the current with the speed of 30-50cm/s is situated in the middle layer over the deep trough. With large tidal fluctuation the volume transport has mean value of 1.17sv which was about 40% larger than that of geostrophic calculation.