• 제목/요약/키워드: Bubble Growth

검색결과 164건 처리시간 0.035초

$CaF_{2}$ 결정의 annealing시 내부 bubbles의 거동 (The behaviour of the internal bubbles in $CaF_{2}$ crystals during the annealing process)

  • 심광보;박대출;주경;오근호
    • 한국결정성장학회지
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    • 제6권4호
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    • pp.595-599
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    • 1996
  • 결정입계를 갖는 $CaF_{2}$ 결정을 annealing할 때, 내부에 존재하는 bubbles의 거동을 결정학적으로 분석하였다. 이들 bubbles는 결정 내에서 일어나는 slip 현상처럼 $CaF_{2}$ 결정구조에 의존하여 특정한 방향으로 배향되어 있음이 확인되었다. 또한, AFM(atomic force microscope)으로 분석한 결과, 이들의 움직임은 negative grain growth에 의한 S-surface를 형성하고 있음이 관찰되었다.

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Computational Fluid Dynamic Simulation of Single Bubble Growth under High-Pressure Pool Boiling Conditions

  • Murallidharan, Janani;Giustini, Giovanni;Sato, Yohei;Niceno, Bojan;Badalassi, Vittorio;Walker, Simon P.
    • Nuclear Engineering and Technology
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    • 제48권4호
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    • pp.859-869
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    • 2016
  • Component-scale modeling of boiling is predominantly based on the Eulerian-Eulerian two-fluid approach. Within this framework, wall boiling is accounted for via the Rensselaer Polytechnic Institute (RPI) model and, within this model, the bubble is characterized using three main parameters: departure diameter (D), nucleation site density (N), and departure frequency (f). Typically, the magnitudes of these three parameters are obtained from empirical correlations. However, in recent years, efforts have been directed toward mechanistic modeling of the boiling process. Of the three parameters mentioned above, the departure diameter (D) is least affected by the intrinsic uncertainties of the nucleate boiling process. This feature, along with its prominence within the RPI boiling model, has made it the primary candidate for mechanistic modeling ventures. Mechanistic modeling of D is mostly carried out through solving of force balance equations on the bubble. Forces incorporated in these equations are formulated as functions of the radius of the bubble and have been developed for, and applied to, low-pressure conditions only. Conversely, for high-pressure conditions, no mechanistic information is available regarding the growth rates of bubbles and the forces acting on them. In this study, we use direct numerical simulation coupled with an interface tracking method to simulate bubble growth under high (up to 45 bar) pressure, to obtain the kind of mechanistic information required for an RPI-type approach. In this study, we compare the resulting bubble growth rate curves with predictions made with existing experimental data.

하우스 종묘삼 재배에서 마이크로 버블(Micro bubble) 사용이 생육에 미치는 영향과 고품질 인삼 가공의 가능성 (Effect of Micro Bubble on Growth of Ginseng in the shaded plastic houses and Possibility of High Quality Ginseng processing)

  • 안철현
    • 현장농수산연구지
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    • 제19권1호
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    • pp.109-117
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    • 2017
  • 아직까지 많이 알려지지 않은 마이크로버블을 사용하여 우리나라 대표 작물인 인삼재배에 적용하였다. 고년근에 적용하여 결과를 확인하기 위해서는 비용과 시간 소요가 많아 종묘삼을 활용하여 생리적 변화를 측정하고 분석하였다. 최근 뿌리 작물에 기능성이 있다는 산소수 일반 재배농가에서 사용해보았지만 그 결과가 미미하고 오히려 해를 입는 경우도 생기게 되었다. 다른 작물의 선행결과와 본 연구결과를 볼 때 마이크로 버블을 사용한 인삼재배는 파급효과 있을 것으로 사료된다. 중화제 및 약제를 활용하여 만든 산소수와는 다른 개념으로 마이크로 버블은 공급 장치를 통해 우리가 이용하는 공기를 아주 작은 버블로 압축하여 인삼에 제공함으로써 저해 없이 특이성 성장을 이끌어 내었다. 연구결과로부터 설정된 종묘삼의 생장 특성 및 세분화별 적정범위 및 적정치를 결과와 비교하면, 그동안 이루어졌던 관행농법에서 사용되는 일반수와 마이크로 버블(Micro bubble)수를 사용하여 재배한 결과는 10%에서 15%의 인삼생장을 나타내었다. 이후로 마이크로 버블수를 생산할 때 시간별 용존 산소량을 측정하여 마이크로 발생장치의 최적 시간을 설정하고 최적화 설정을 위해서는 관계시간과 에너지 효율 및 토양의 영양환경에 대한 변화에 대해서도 더욱 많은 연구가 필요하고 사료되며, 더불어 생체 및 중량이 증가된 만큼 인삼의 주요 성분인 진세노사이드의 증감에 대한 분석 등 추가 연구가 활발하게 이루어져야 할 것이다.

병렬 미세관에서의 기포성장 및 역류현상에 관한 수치적 연구 (Numerical Study of Bubble Growth and Reversible Flow in Parallel Microchannels)

  • 이우림;손기헌
    • 대한기계학회논문집B
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    • 제32권2호
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    • pp.125-132
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    • 2008
  • The bubble dynamics and heat transfer associated with nucleate boiling in parallel microchannels is studied numerically by solving the equations governing conservation of mass, momentum and energy in the liquid and vapor phases. The liquid-vapor interface is tracked by a level set method which is modified to include the effects of phase change at the interface and contact angle at the wall. Also, the reversible flow observed during flow boiling in parallel microchannels has been investigated. Based on the numerical results, the effects of contact angle, wall superheat and the number of channels on the bubble growth and reversible flow are quantified.

Modeling of Atomization Under Flash Boiling Conditions

  • Zeng, Yangbing;Lee, Chia-Fon
    • 한국연소학회지
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    • 제7권1호
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    • pp.44-51
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    • 2002
  • This paper presents an atomization model for sprays under flash boiling conditions. The atomization is represented by the secondary breakup of a bubble/droplet system, and the breakup is considered as the results of two competing mechanisms, aerodynamic force and bubble growth. The model was applied to predict the atomization of a hollow-cone spray from pintle injector under flash boiling conditions. In the regimes this study considered, sprays are atomized by bubble growth, which produces smaller SMD#s than aerodynamic forces alone. With decreasing ambient pressures, the spray thickness, fuel vaporization rate and vapor radial penetration increases, and the drop size decreases. With increasing the fuel and ambient temperatures to some extent, the effect of flash boiling and air entrainment completely change the spray pattern.

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Numerical simulation of bubble growth and liquid flow in a bubble jet micro actuator

  • Ko, Sang-Cheol;Park, Nam-Seob
    • Journal of Advanced Marine Engineering and Technology
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    • 제38권10호
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    • pp.1232-1236
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    • 2014
  • Numerical models of fluid dynamics inside the micro actuator chamber and nozzle are presented. The models include ink flow from reservoir, bubble formation and growth, ejection through the nozzle, and dynamics of refill process. Since high tapered nozzle is one of the very important parameters for overall actuator performance design. The effects of variations of nozzle thickness, diameter, and taper angles are simulated and some results are compared with the experimental results. It is found that the ink droplet ejection through the thinner and high tapered nozzle is more steady, fast, and robust.

마이크로 히터에서의 기포성장과 온도변화에 관한 실험적 연구 (An Experimental Study on Bubble Growth and Temperature Change on Microheater)

  • 고승현;김호영;김신규;장영수;이윤표;김용찬
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2003년도 추계학술대회
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    • pp.1010-1015
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    • 2003
  • Bubble growth on microheater has been experimentally investigated in this study. The experiment was performed using platinum microheaters having dimensions of 300 ${\mu}m$ or 50 ${\mu}m$ in length, 20 ${\mu}m$ or 5 ${\mu}m$ in width, and $0.2{\pm}0.01$ ${\mu}m$ in thickness. A high speed video camera was used to observe bubble growth at 2,000 frames per second. Microheater temperature was measured at the rate of 300 Hz. with a data acquisition system. Bubble nucleation frequency increased with working fluid temperature. Although the slope of temperature drop was similar in all cases, the magnitude of temperature drop was different. The temperature profiles and the high speed camera images were combined to explain temperature drop.

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마이크로 엑츄에이터의 설계변수에 따른 유동특성 해석 (Numerical analysis of liquid flow characteristics according to the design parameters of a bubble jet microactuator)

  • 고상철
    • Journal of Advanced Marine Engineering and Technology
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    • 제40권7호
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    • pp.605-612
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    • 2016
  • 버블젯 타입 마이크로 엑츄에이터의 설계변수에 따른 유동특성에 관한 수치해석적 연구를 수행하였다. 수치 모델은 저장소로 부터의 잉크 유동과 기포의 성장 및 소멸, 노즐을 통한 액적의 토출과 리필 과정을 포함한다. 기포의 거동은 전체 엑츄에이터의 성능에 중요한 영향을 미치는 요소이기 때문에, 본 연구에서는 open pool 해석을 통하여 기포의 성장과 소멸 및 소멸시의 캐비테이션 현상에 대해 살펴보았다. 또한 마이크로 엑츄에이터의 노즐 형상의 변화, 챔버와 리스트릭터의 기하학적 변화에 따른 액적의 토출과 잉크 리필과정에 대한 수치예측을 수행하였다. 설계변수의 변화에 따른 수치해석의 결과는 마이크로 엑츄에이터의 성능특성을 예측할 수 있으며 또한 마이크로 엑츄에이터의 최적설계에 유용하리라 판단된다.

Numerical Simulation of Cavitating Flows on a Foil by Using Bubble Size Distribution Model

  • Ito, Yutaka;Nagasaki, Takao
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2004년도 제22회 춘계학술대회논문집
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    • pp.216-227
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    • 2004
  • A new cavitating model by using bubble size distribution based on bubbles-mass has been proposed. Both liquid and vapor phases are treated with Eulerian framework as a mixture containing minute cavitating bubbles. In addition vapor phase consists of various sizes of vapor bubbles, which are distributed to classes based on their mass. The bubble number-density for each class was solved by considering the change of the bubble-mass due to phase change as well as generation of new bubbles due to heterogeneous nucleation. In this method, the bubble-mass is treated as an independent variable, and the other dependent variables are solved in spatial coordinates and bubble-mass coordinate. Firstly, we employed this method to calculate bubble nucleation and growth in stationary super-heated liquid nitrogen, and bubble collapse in stationary sub-cooled one. In the case of bubble growth in super-heated liquid, bubble number-density of the smallest class based on its mass is increased due to the nucleation. These new bubbles grow with time, and the bubbles shift to larger class. Therefore void fraction of each class is increased due to the growth in the whole class. On the other hand, in the case of bubble collapse in sub-cooled liquid, the existing bubbles are contracted, and then they shift to smaller class. It finally becomes extinct at the smallest one. Secondly, the present method is applied to a cavitating flow around NACA00l5 foil. Liquid nitrogen and liquid oxygen are employed as working fluids. Cavitation number, $\sigma$, is fixed at 0.15, inlet velocities are changed at 5, 10, 20 and 50m/s. Inlet temperatures are 90K in case of liquid nitrogen, and 90K and 1l0K in case of liquid oxygen. 110K of oxygen is corresponding to the 90K of nitrogen because of the same relative temperature to the critical one, $T_{r}$=$T/T_c^{+}$. Cavitating flow around the NACA0015 foils was properly analyzed by using bubble size distribution. Finally, the method is applied to a cavitating flow in an inducer of the LE-7A hydrogen turbo-pump. This inducer has 3 spiral foils. However, for simplicity, 2D calculation was carried out in an unrolled channel at 0.9R cross-section. The channel moves against the fluid at a peripheral velocity corresponding to the inducer revolutions. Total inlet pressure, $Pt_{in}$, is set at l00KPa, because cavitation is not generated at a design point, $Pt_{in}$=260KPa. The bubbles occur upstream of the foils and collapse between them. Cavitating flow in the inducer was successfully predicted by using the bubble size distribution.

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