• 오토저널
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• 제14권5호
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• pp.41-53
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• 1992

The main purpose of this study is to investigate the atomizing characteristics of a two phase spray by using a liquid column type coaxial nozzle. The experiments have been carried out to analyze the atomization behavior, the droplet size distributions, and the statistical properties of droplet size distributions. Immersion sampling method and the image processing technique were adapted for the measurements of particles, and the distributions of the droplet sizes were statistically analyzed. In the experiments, the mass ratio defined as Mr= $M_{\sigma}$/ $M_{1}$ has been changed from 1.0 to 3.4 and the measurements have been performed along the axis of the spray. As a result of this experimental study, the distributions of droplet size were satisfied with the Log-Normal distributions and arithmetic mean diameter and deviation of mass ratio. Droplet volume-surface mean diameter was denoted by a exponential function of mass-ratio and the exponent was denoted by linear relation according to the central axis from the nozzle. Dispersions, skewness factors and flatness factors had comparatively constant values regardless of mass ratio and location.

• 공업화학
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• 제25권2호
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• pp.181-187
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• 2014

구형의 아토마이징 제강 환원슬래그(래들로 슬래그)를 폴리머 콘크리트 복합재료의 잔골재 대신 사용하기 위하여 아토마이징 제강 환원슬래그의 대체율과 폴리머 결합재의 첨가율을 다양하게 변화시켜 공시체를 제작하였다. 공시체의제 물성을 조사하기 위하여 흡수시험, 압축 및 휨강도, 내열수성시험, 세공분포측정 및 SEM에 의한 미세조직 관찰을 실시하였다. 그 결과 폴리머 결합재 7.5% 첨가한 공시체는 제강 환원슬래그의 대체율이 증가됨에 따라 압축 및 휨강도가 증가되었으나 폴리머 결합재 8.0% 이상에서는 유동성의 증가로 인한 재료분리 현상으로 특정한 대체율에서 최대값을 나타내었다. 내열수성시험에 의하여 압축강도, 휨강도, 세공의 평균직경 및 밀도는 감소되었으나 총세공량과 공극률은 증가되었다. 아토마이징 제강 환원슬래그를 잔골재 대신 사용함으로써 유동성이 현저히 증가되어 폴리머 결합재의 사용량을 최대 23.5%까지 절감할 수 있는 것으로 나타났다. 그러나 아토마이징 제강 환원슬래그를 사용함으로써 내열수성이 감소되기 때문에 더 많은 연구가 요구된다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집D
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• pp.528-533
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• 2001

An experimental study is carried out to investigate the effects of air and water mass flow rates on cooling characteristics of mist impinging jet on a flat plate. Experiments are conducted with air mass flow rates from 0.0 to 3.0 g/s, and water mass flow rates from 5.0 to 20.0 g/s. An air-atomizing nozzle is used for the purpose of controlling air and water mass flow rates. In this study, a new test section is designed to obtain local heat transfer coefficient distributions. Heat transfer characteristics of the mist impinging jet are explained with the aid of flow visualization. Surface temperature and heat transfer coefficient distributions become more uniform as air mass flow rate increases, and that the increases in water flow rate mainly enhance cooling performance. Air mass flow rate weakly influences averaged heat transfer coefficient when water mass flow rate is low, but averaged heat transfer coefficient increases remarkably as air mass flow rate in case of high water mass flow rate.

• 대한기계학회논문집B
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• 제27권4호
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• pp.511-517
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• 2003

An experiment is conducted to investigate the effect of air and water mass flow rates on cooling characteristics of mist impinging jet on a flat plate. The air mass flow rate ranges from 0.0 to 3.0 g/s, and water mass flow rates from 5.0 to 20.0 g/s. An air-atomizing nozzle is used fur the purpose of controlling air and water mass flow rates. The test section is designed distinctively from previous works to obtain local heat transfer coefficient distributions. Heat transfer characteristics of the mist impinging jet are explained with the aid of flow visualization. Surface temperature and heat transfer coefficient distributions become more uniform as air mass flow rate increases. The water flow rate provides substantial contribution to enhancement of cooling performance. On the other hand, The air mass flow rate weakly influences the averaged heat transfer rate when the water mass flow rate is low, but the averaged heat transfer rate Increases remarkably with the air mass flow rate in case of the high water mass flow rate.

• Journal of Biosystems Engineering
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• 제21권4호
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• pp.467-473
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• 1996

Ultrasonic energy was applied for atomizing rice-bran oil which is a highly viscous bio fuel. Six different nozzles, an injection simulator, and an ultrasonic generator system were designed and constructed for the experiment. An immersion liquid method was used for the measurement of injection droplet sizes. The characteristics of injection droplets was investigated with respect to the numbers of the droplets with diameters ranging from 5$\mu$m 50$\mu$m and to the Sauter mean diameter. The results showed that the ultrasonic energy was effective for the improvement of the atomization of the injection droplets for all the factors such as type of nozzles, nozzle opening pressures, and collection distances.

• 대한화장품학회지
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• 제37권1호
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• pp.43-53
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• 2011

여드름 나노화장품(nanocosmetics) 개발을 위하여 azelaic acid-milk nano powder의 nanoencapsulation을 fluid-bed processor로 중심합성계획에 따라 유입공기온도($60{\sim}80^{\circ}C$) 분무속도(0.5 ~ 0.9 mL/min) 및 분무압력(1.2 ~ 2.0 kg/$cm^2$)을 달리하여 나노캡슐(nanoencapsule)을 제조하고, 나노캡슐의 품질특성을 조사하여 회귀분석을 실시하였다. 나노캡슐의 예측된 수율의 최대값은 70.97 %로 수율은 유입공기온도, 분무속도 및 분무압력 에 의해 크게 영향을 받고 있었다. 시료의 입자크기는 유입공기온도가 높고 분무속도가 빠르며, 분무압력이 낮을수록 커지는 것으로 나타났고, 생리식염수에서 나노캡슐의 용출율은 모두 유입공기온도 및 분무속도에 의해서 가장 많은 영향을 받고 있었다. 수분함량은 분무 속도가 증가하고 분무압력이 높아질수록 증가하였고, 수분활성도는 수분함량과 유사한 경향을 나타내었다. 기계적 색도인 L값과 b값은 유입공기온도가 높아질수록 증가하였다. 수율이 높고 입자크기가 작으며, 피부적합성 나노캡슐 제조의 최적조건은 유입공기온도 $67{\sim}73^{\circ}C$, 분무속도 0.6 ~ 0.8 mL/min 및 분무압력 1.8 ~ 2.0 kg/$cm^2$ 범위로 예측되었다. 이상의 예측범위 내의 임의의 점에서실제 실험한 실험치는 반응표면분석법에 의해 예측된 값과 유사한 경향을 보여 도출된 회귀식의 신뢰성을 검증할 수 있었다.

• 한국세라믹학회지
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• 제32권5호
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• pp.549-558
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• 1995

Mn-Zn ferrite granules were prepared by spray drying of the slurry containing different kinds and concentration of binders at various spray drying temperatures and atomizing pressures. The characteristics of the spraydried granules were analyzed according to the processing variables of spray drying and the slurries containing different solid loading and kinds and concentration of binders. Typical shape of the spray dried granules was spherical. The granules spray dried at 15$0^{\circ}C$ were more spherical and containing lower hollow percentage than any other granules prepared at higher temperature. The granules prepared at higher atomizing pressures were more spherical and become smaller in size. The granules prepared using slurry containing higher solid loading were larger in size and less defective in shape. As increasing the concentration of binder the number of donut-shaped granules was increased and the size distribution become broader. The granules prepared using the slurry containing PVA 205 were more spherical than those containing PVA 217 and PVA 117. As the amount of granules which were donut-shaped or dimpled increased the compaction response were less effective. The hollows were not fractured completely even at hight pressures and remained after sintering.

• 한국분말야금학회:학술대회논문집
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• 한국분말야금학회 2006년도 Extended Abstracts of 2006 POWDER METALLURGY World Congress Part 1
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• pp.451-452
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• 2006

The influence of Hi-flux powders characteristics on the performance of magnetic powder cores was studied. It was found that different cooling rate and nozzle configuration could change the shape and microstructure of powders. Smooth surface and spherical shape of powders were beneficial to improve DC bias performance and reduce core losses of magnetic powder core.

• 청정기술
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• 제9권4호
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• pp.163-168
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• 2003

회전형 도장기기의 핵심 부품인 공기 터빈 및 무화 디스크 설계를 위한 기본 설계개념 및 방법을 제시하였고, 이를 이용하여 도장기기를 설계, 제작하였다. 제작된 도장기기의 회전수 및 유량의 측정 결과는 전산유체역 학적 해와 잘 일치하였다. 또한 공기 터빈 및 디스크 설계 사양에 따라 도장기기의 회전수가 현저히 변화됨을 알 수 있었고, 공기 터빈의 유로 기울기 $20^{\circ}$, 노즐 수 2개일 때의 도장기기 성능이 가장 우수하였다.

• 한국분무공학회지
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• 제4권1호
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• pp.19-26
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• 1999

An experimental study of twin-fluid atomization for powder metallurgy has been conducted using a specially designed atomizer in which liquid is first spread into a thin sheet and then exposed on both sides to high-velocity air. Inner air jet worked for supplying liquid and outer air jets disintegrated liquid sheet. The first result of this study were confined to the effect of atomizing quality through experiments with water. The experimental data will be extend to include the influence of atomizing air velocities on mean particle size through experiments with molten material. An experimental equation on the relationship between SMD and the related parameters was taken out; $$SMD=0.00302\frac{{(\sigma_L\;\rho_L\;D_L)}^{0.5}}{\rho_A(V_1+1.155\;V_2)/2}(1+\frac{W_L}{(W_{A1}/3.33)+W_{A2}})+0.0148(\frac{{\mu_L}^2}{\sigma_L\;\rho_L})^{0.425} \;{D_L}^{0.575}(1+\frac{W_L}{(W_{A1}/3.33)+W_{A2}})^2$$.