The properties of pyrolytic carbon (PyC) deposited from C2H2 and a mixture of C2H2/C3H6 on ZrO2 particles in a fluidized bed reactor were studied by adjusting the deposition temperature, reactant concentration, and the total gas flow rate. The effect of the deposition parameters on the properties of PyC was investigated by analyzing the microstructure and density change. The density could be varied from 1.0 g/cm3 to 2.2 g/cm3 by controlling the deposition parameters. The density decreased and the deposition rate increased as the deposition temperature and reactant concentration increased. The PyC density was largely dependent on the deposition rate irrespective of the type of the reactant gas used.

Costal regions in Korea often suffer severe damages due to wave-induced disasters, storm surge disasters and so on. therefore, many engineers and researchers have devoted their energy to prevent these costal disasters. The development of artificial reefs including sunken vessels is one of their remarkable achievements and various kind of these artificial upwelling structures have been designed and applied. However, the flow characteristics around a Tetrapod under the water has not been investigated experimentally. So in this article, in uniform flow of circulating water channel and some different velocities, PIV measurement has been conducted on the flow characteristics behind a Tetrapod. The results were analyzed on the flow characteristics of both cases of a Tetrapod. Therefore, it can be concluded that the both cases have its own distinctive flow characteristics behind the bluff body; Case A has an steep upstream flow pattern. On the contrary, Case B has an developed downstream flow pattern in the near wake of the Tetrapod. The velocity gradient at position x=150mm of Case-A appears gently up and down But, the velocity gradient at the same position of Case-B appears better highly up and down.

삼각형상 구조물은 바다에서 풍요로운 어장을 만들기 위해 용승류를 발생시키기 위한 인공용승구조물의 기본적인 형태로 이용되고 있다. 인공용승류는 많은 양의 영양염류를 포함하고 있는 저층의 바닷물을 해저로부터 표층으로 끌어 올리는 작용을 한다. 이 연구의 목적은 여러 가지 성층계수에 따른 삼각형상 수중구조물 주위의 유동특성을 규명하는 것이다. 회류수조 내에서 삼각형상 구조물 모델을 대상으로 유동특성을 조사하기 위하여 유동가시화 방법을 이용한 실험적 연구를 수행하였고, 입자영상유속계(PIV)를 이용하여 수중구조물 주위의 유동장을 계측하였다. 실험결과 구조물 후상부 영역에서의 용승효과는 수심이 구조물 높이의 2배이고, 성층계수가 약 3.0일 때 가장 좋은 결과가 나타났다. 이러한 정량적인 데이터는 인공용승구조물의 기능적 효율을 결정하는 데에 유용하게 이용될 수 있을 것이다.

난류 경계층 유동과 물체주위의 상관유동 및 그 물체 주위에서의 부압 생성과 관련, 그 유동특성에 대한 이해를 높이기 위하여 두꺼운 난류 경계층 내에 놓인 큐브물체 주위의 박리유동에 대해 연구를 수행하였다. 2차원의 PIV와 열선유속계를 이용하여 풍동 내에서 두꺼운 경계층을 생성시키는 실험이 수행되었다. 실험은 큐브의 높이 h에서 측정된 유속 U에 근거한 레이놀즈 수 18,600에서부터 349,000 의 범위에서 수행되었으며, 이 레이놀즈 수의 범위는 평균유동이 레이놀즈 수와 관계없이 충분히 크다고 판단된다. 본 연구에서 큐브의 선단주위와 상부에서의 유동장 측정결과들을 제시할 것이다. 연구결론으로 레이놀즈 효과는 평균표면압력이라든지 표면근처의 평균유속과 같은 평균유동특성에 별 영향을 미치지 않았지만, 섭동장은 큰 영향을 나타내고 있었다.

The paper concerns an experimental and numerical study of fully developed laminar flow of a Newtonian, water and non-Newtonian fluids, 0.2% aqueous of sodium carboxymethyl cellulose(CMC) solution in concentric and eccentric annuli with combined bulk axial flow and inner cylinder rotation. Pressure losses and skin friction coefficients have been measured when the inner cylinder rotates at the speed of 0～300 rpm. The influences of rotation, radius ratio and working fluid on the annular flow field are investigated.

버터플라이 밸브는 선박에서 냉각수와 유류 계통 등에 범용으로 널리 사용되고 있다. 이 연구에서는 유량조정에 따른 배관계통의 버터플라이밸브 후류 유동특성을 규명하기 위하여 입자영상 유속측정장치를 이용하여 밸브개도에 따른 유선과 속도벡터 분포에 관한 정량적인 데이터를 확보하였다. 또한 밸브 주위 유동장의 압력성분을 고찰하기 위하여 개폐각도를 6가지 경우로 변화시켜 정압을 측정하였다. 그 결과 실험관 벽면에서 측정된 압력의 분포는 디스크가 전개 상태인 0˚에서 45˚까지는 입구 압력은 일정한 상태로 거의 변화하지 않았으나 약 60˚ 이상에서부터 압력 상승과 점차 급격한 변동현상이 나타났다. 특히, 75˚ 부근에서는 상류에서 급격한 압력 상승 경향을 보인 반면 하류 측은 압력변동이 적게 나타났다.

이 연구에서는 실제선박의 후드룸을 1/15로 축소한 비대칭 입출구를 갖는 장방형 모델을 대상으로 가시화 실험을 수행하고 내부의 유동 특성을 고찰하고자 하였다. 속도장의 계측은 CACTUS'2000을 이용한 2차원 PIV기법으로 하였으며 4개의 계측영역을 설정하여 계측한 결과 유동장의 환기구조를 지배하는 흐름은 유동장의 좌측 벽면의 흡기구로부터 대각방향의 우측상부로 흐르는 나선형의 'L'형 유동이었다. 또한 주 흐름의 영향으로 유동장의 중앙부분에 강제와류형태의 재순환 흐름이 존재하였다.

This research aims at establishing the fundamental characteristics of the kite through the analysis of the flow field around various types of kites. The approach of this study were adopted for the analysis; visualization by CFD(computational fluid dynamics). Also, the lift/drag and PIV(particle image velocimetry) tests of kites had been performed in our previous finding. For this situation, models of canvas kite were designed by solidworks(design program) for the CFD test using the same conditions as in the lift/drag tests. And we utilized FloWorks as a CFD analysis program. The results obtained from the above approach are summarized as follows: According to comparison of the measured and analyzed results from mechanical tests, PIV and CFD test, the results of all test were similar. The numerical results of lift-coefficient and drag-coefficient were 5-20% less than those of the tests when attack angle is 10˚, 20˚ and 30˚. In particular, it showed the 20% discrepancy at 40˚. The numerical results of the ratio of drag and lift were 8-13% less than those of the tests at 10˚ and 10% less than those of the tests at 20˚, 30˚ and 40˚. Pressure distribution gradually became stable at 10˚. In particular, the rectangular and triangular types had the centre of the high pressure field towards the leading edge and the inverted triangular type had it towards the trailing edge. The increase of the attack angle resulted in the eddy in order of the rectangular, triangular and inverted triangular type. The magnitude of the eddy followed the same order. The effect of edge-eddy was biggest in the triangular type followed by the rectangular and then the inverted triangular type. The action point of dynamic pressure as a function of the attack angle was close to the rear area of the model with the small attack angle, and with large attack angle, the action point was close to the front part of the model.

This research aims at establishing the fundamental characteristics of the kite through the analysis of the flow field around various types of kites. The approach of this study were adopted for the analysis; visualization by PIV(particle image velocimetry). Also, the lift and drag tests of kites had been performed in our previous finding(Bae et al., 2004a; Bae et al., 2004b). For this situation, models of canvas kite were deployed in the circulating water channel for the PIV test using the same conditions as in the lift and drag tests. The results obtained from the above approach are summarized as follows: Given the rectangular and triangular kites when attack angle is 20˚, vortex by the boundary layer separation was seen in the leading edge and the flow towards the trailing edge was more turbulent. But, the inverted triangular type kite was seen to be stable without any boundary layer separation or turbulence. The increase of the attack angle resulted in the eddy in order of the rectangular, triangular and inverted triangular type. The magnitude of the eddy followed the same order. The effect of edge-eddy was biggest in the triangular type followed by the rectangular and then the inverted triangular type. The kite as the buoyancy device or the opening device will be very useful when the appropriate applications and the stability are met.

The characteristics of fluidized bed catalytic combustion for sludge treatment have been studied in a pilot scale of fluidized bed combustor. 1.0wt% Pt of catalyst supported on the spherical alumina was mixed with the spherical pure alumina as a bed material. Sewage sludge, heating value of which is 3,440 kcal/kg, was used as a waste sample in the experiment. Through the experiments, the various characteristics such as a bed temperature profile and flue gas(CO, SO2) concentration profile were investigated and the catalyst mixing ratio and sample feed rate were applied as experimental parameters. The experimental results showed that bed temperature was maintained more highly and flue gas concentration decreased with the increase of the catalyst mixing ratio, and bed temperature was maintained more highly also and flue gas concentration increased with the increase of the sample feed rate. The combustion efficiency of fluidized bed catalytic combustion of the sludge increased with the increase of the catalyst mixing ratio and sample feed rate and reached more than 96%.