• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2008년도 춘계학술대회논문집
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• pp.185-188
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• 2008

In this study, we experimentally investigated that the optimization of pulsating jet to reduce the separated flow region behind the vertical fence. The vertical fence was submerged in the turbulent boundary layer in the circulating water channel and we applied phase averaged PIV method to measure the instantaneous velocity fields around the fence. One cycle of pulsating jet is divided into 20 phases and grabbed total 200 instantaneous velocity fields at each phase. The experiments were performed by varying the frequency, maximum jet velocity and the shape of pulsating jet wave. Pulsating jet was precisely made by piston-type pump controlled by the computer. The obtained results were compared with normal fence flow. From this study, we found there is the specific frequency which is effective in reducing the reattachment region.

• 정보저장시스템학회논문집
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• 제1권1호
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• pp.48-52
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• 2005

The research topic of super-RENS technology is shifting from the signal intensity (CNR; Carrier to Noise Ratio) to the signal uniformity (Jitter or bER). To achieve an uniform signal characteristics, it is important to reduce signal fluctuation in a super-RENS disc. In this study, we investigated the relation between signal fluctuation and low frequency noise (LFN), and analyzed LFN increase in recording and readout processes. It was found that signal fluctuation had a close relationship with the LFN. Also, it was found that the recorded mark shape such a bubble type and high readout power increased the LFN in recording and readout process of a super-RENS disc. So, using non-bubble type recording material and low super-resolution readout material, we markedly improved the LFN in a super-RENS disc.

• 설비공학논문집
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• 제14권2호
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• pp.108-115
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• 2002

The fundamental mechanism of a dispersed two-phase flow was investigated. Experiments were carried out to understand how the particles behaves under the influence of the particle size, shape, metamorphoses (bubble) and buoyancy of a single particle which is ascending from the standstill water. Two CCD cameras were employed for image processing of the behavior of the particles and the surrounding flow, which was interpreted with the technique of correlation PIV (Particle Image Velocimetry) and PTV (Particle Tracking Veloci- metry), respectively The experimental results showed that the large density difference bet- ween a particle and water caused high relative velocity and induced zigzag motion of the particle. Furthermore, the turbulence intensity of a bubble was about twice the case of the spherical solid particle of similar diameter.

• 한국수소및신에너지학회논문집
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• 제28권2호
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• pp.121-128
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• 2017

For an investigation on the effect of the shape of electrodes in alkaline water electrolysis, two kinds of stack with circular and square electrode array are used to visualize both for behaviors of hydrogen bubble around the electrodes and for measurements of hydrogen production from these two stacks. The electrolytes for the hydrogen production experiment were applied for 20 wt%, 25 wt%, 30 wt% and 35 wt% of KOH alkaline aqueous solutions. As a result, the adhesion length of bubbles attached around the square electrode in the visualization experiment was found to be 1.7 times longer compared with the attached around the circular electrode. In the hydrogen production experiments, the volume of hydrogen production of the stack by using circular electrode array was approximately 3% more than that of the stack with square electrode array. These observations may be caused by the effect of the bubbles attached to the around the electrodes obstructing mass transfer such as hydrogen exhaust and electrolyte supply.

• 한국음향학회지
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• 제33권1호
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• pp.10-20
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• 2014

본 연구에서는 입수 충격에 의한 수중 순간 소음을 연구하기 위해, 황해에서 발사대를 이용하여 해상 실험을 진행하였다. 해상시험선인 청해호 우현상에서 발사대를 이용하여 실린더 몸체를 수직으로 발사하였으며, 이때 발생하는 소음을 하이드로폰으로 측정하였다. 실험에서는 원통형, 원뿔형, 반구형 두부 형상을 가진 3가지 종류의 실린더 몸체가 사용되었다. 측정된 신호는 시간적으로 확연하게 구분되어 3단계로 전시되었다 : (1) 초기 충돌 및 물체 진동단계, (2) 개방 공동 유동 단계, (3) 공동 붕괴 및 거품 진동 단계. 대부분의 경우, 거품 진동 단계의 파형이 초기 충돌 및 물체 진동 단계에 비해 우세하게 나타났다. 공동이 붕괴되기 시작하는 핀치 오프 시간은 0.18 ~ 0.2 s에 발생하였으며, 평균 거품 지속 시간은 0.9 ~ 1.3 s로 지속되었다. 입수 충격 소음은 100 Hz 이하의 대역에서 에너지가 집중되어 있었으며, 생성되는 소음은 두부 형상, 물체 질량, 발사 속도에 의해 영향을 받았다. 결과적으로, 거품 주파수에서 에너지 스펙트럼 밀도의 크기는 원통형, 원뿔형, 반구형 순으로 나타났으며, 동일 입수체에 대해서는 초기 에너지가 클수록 거품 주파수에서 에너지 스펙트럼 밀도가 크게 나타났다. 최종적으로, 버블이 폭발하는 물리적 현상을 기반으로 모의된 신호와 계측 값간 비교 결과 만족스러운 결론을 얻을 수 있었다.

• The Journal of the Acoustical Society of Korea
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• 제29권1E호
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• pp.28-37
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• 2010

This article reviews recent developments in the emerging field of cellular-level biomedical ultrasonics with the specific focus on the mechanics of ultrasound-cell interaction. Due to the nature of the field at its relative infancy, the review poses more questions than it provides answers. Discussed are topics such as the basic structure of a biological cell, the origin of cell's elasticity, a theoretical framework for ultrasound-cell interaction, and shape deformation of cells and its measurement, Some interesting problems for future study are proposed.

• 한국균학회지
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• 제31권2호
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• pp.89-93
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• 2003

송이균사의 대량배양에 적합한 공기부양식 생물반응기 형태를 찾고자 풍선형 및 칼럼형의 공기부양식 생물반응기와 external-loop형의 기포통기식 생물반응기에서 송이균사체를 심부배양하여, 반응기 형태별 송이균사체의 생장특성을 비교하였고, 반응기 형태가 세포에 주는 스트레스 정도를 비교하기 위하여 배양기 형태별 균사체의 에르고스테롤의 함량 변화를 비교하였다. 반응기 형태별 송이 균사체의 생산량은 풍선형 생물반응기에서 평균 12g, external-loop형의 기포통기식 생물반응기에서 평균 11.4g, 칼럼형 생물반응기는 평균 9.5g을 생산하여, 풍선형 생물반응기가 가장 우수하였다. 생장기간도 풍선형 생물반응기에서 균사 접종 후 16일 이후부터 정체기에 이르는 것으로 20일 이후에 나타난 칼럼형 및 기포통기형 생물반응기 보다 빠르게 생장하는 것으로 나타났다. 균사체의 생장시기별 에르고스테롤의 함량은 풍선형 공기부양식 생물반응기에서 가장 높이 나타났으며 이어서 칼럼형, 기포통기식 순으로 나타나, 송이 균사체 배양시 반응기 형태에 의한 물리적 스트레스는 풍선형 공기부양식 생물반응기가 가장 적게 받는 것으로 추정되었다. 송이 균사체 배양에 가장 적합한 공기부양식 생물반응기의 형태는 풍선형인 것으로 추정 할 수 있었다. 그러나 칼럼형 및 풍선형 공기부양식 생물반응기는 스파자 부근에서 균사체가 침적, 착생하여 점차 크게 뭉쳐 성장하면서 공기공급을 차단하는 현상이 있었으나 external-loop형의 기포통기식 생물반응기에서는 유체의 순환으로 이러한 현상은 적게 나타나 대용량의 송이 균사체 배양에 적합한 반응기 형태로는 배양기의 상부가 풍선형 반응기의 형태를 유지하고, 스파자가 위치한 하부는 external-loop형의 기포통기식 생물반응기의 유체 순환식 형태를 유지하도록하는 혼합형의 형태가 좋을 것으로 추정되었다.

• 한국정밀공학회지
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• 제31권1호
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• pp.75-81
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• 2014

Laser beam machining has been known as efficient for glass micromachining. It is usually used the ultra-short pulsed laser which is time-consuming and uneconomic process. In order to use economic and powerful long pulsed laser, indirect processing called laser-induced backside wet etching (LIBWE) is good alternative method. In this paper, micromachining of glass using Nd:YAG laser with nanosecond pulsed beam has been attempted. In order to improve shape accuracy, combined processing with magnetic stirrer has been widely used. Magnetic stirrer acts to circulate the solution and remove the bubble but it is not suitable for deep hole machining. To get better effect, ultrasonic vibration was applied for improving shape accuracy.

• 한국전기전자재료학회논문지
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• 제18권9호
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• pp.798-802
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• 2005

The plating shape in the opening of photoresist becomes gradated shape in the fountain plating system, because bubbles from the wafer surface are difficult to escape from the deep openings, vias. In this paper, the bubble flow from the wafer surface during plating process was studied and we designed the tilted electrode ring to get uniform bump height on all over the wafer and evaluated the film uniformity by SEM and $\alpha-step$. In a-step measurement, film uniformities in the fountain plating system and the tilted electrode ring contact system were $\pm16.6\%,\;\pm4\%$ respectively.

• 한국전산유체공학회지
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• 제14권3호
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• pp.63-68
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• 2009

The motion of a rising liquid droplet is different that of a bubble motion. Treatment of liquid drops is more complex because internal motion must be considered. A 3D unstructured CFD code has been developed to solve incompressible N-S equation for the droplet simulation. This front-tracking consideration which the interface is tracked explicitly is very available to apply for not only exact interface topology but also the high schmidt number issue, such as $CO_2$ dissolution. This paper is forced on the zig-zag motion of the liquid droplet. The simulation shows that if the rising droplet is located at the corner of the zig-zag path, the velocity is low and shape of the droplet is more spherical shape, results in the less drag coefficient. Twin horse shoe vortexes behind the rising droplet are presented and the topology of the droplet is compared with an experimental result during one period of the path.