• Title/Summary/Keyword: 분열기구

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An Experimental Study on Breakup Mode of Epoxy Paint Discharging from a Fan Spray Nozzle (선형분무노즐로부터 분무되는 에폭시계 도료의 분열기구에 대한 실험적 연구)

  • Kang, S.I.;Lee, S.Y.;An, S.M.;Ryu, S.U.
    • Journal of ILASS-Korea
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    • v.12 no.3
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    • pp.138-145
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    • 2007
  • In the present work, the breakup mechanism of highly viscous epoxy paints discharged from a fan spray nozzle was examined experimentally. The paints tested were non-Newtonian fluids, composed of epoxy resin, solid particles and other additives. The paint spray discharged from the nozzle was visualized and recorded using a digital camera with back illumination. Due to presence of the solid particles, perforation of liquid sheet was observed in most cases, even at low-Reynolds number conditions (Re < 15,000) where the aerodynamic-wave breakup mode is used to be dominant for pure liquids. However, with the increase of the particle concentration, the sheet became longer and the thickness at breakup became thinner to some extent. This is because, with higher concentration of solid particles, the stabilizing effect by the viscosity increase predominates over the destabilizing effect by perforation.

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The study of the breakup mechanism of a liquid jet by using a high speed camera (고속도카메라에 의한 액주의 분열기구에 관한 연구)

  • 김덕줄;이충원
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.13 no.4
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    • pp.708-716
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    • 1989
  • The purpose of this study is to investigate the breakup mechanism of a liquid jet in a coaxial air flow. By using the high speed camera, measured were the instantaneous change of the wave length, amuplitude of disturbance, propagation velocity of wave and breakup length, and the relationships between those data were examined. The shape of the surface of the liquid jet appeared to be rather complicated and irregular. The growth rate of disturbance was not constant, and was changed at the moment of 3ms prior to the disintegration of the liquid jet. Simultaneously at this moment, the propagation velocities of the sequential waves were reversed and the wave length was rapidly decreased.

A Study on Analysis of Breakup Mechanism of Vaporizing Fuel Droplet in High Temperature and Velocity Air Stream (고온고속류에서 기화를 고려한 연료액적의 분열(Breakup)기구 해석에 관한 연구)

  • Kim, K.C.;Hwang, S.S.
    • Journal of ILASS-Korea
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    • v.3 no.3
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    • pp.1-13
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    • 1998
  • In this study, an experimental study was performed to investigate the breakup mechanism of vaporizing droplet. A well-controlled experimental apparatus was used to study breakup mechanisms of a monodisperse stream of drops injected into a transverse high temperature and velocity air stream. The experiments gave information$ about the microscopic structure of the liquid drop breakup process, drop breakup regimes, and drop trajectories in high temperature flow region. The breakup time, drop acceleration and wavelength of surface instability wave were measured from a high-magnification and double spark photography. The two instability theories, i.e., Kelvin-Helmholtz instability and Rayleigh-Taylor instability, were estimated by comparing the calculated data with the measurements. The results showed that the breakup time in high temperature flow condition is shortened because the surface tension is decreased by the increase of gas temperature.

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The influence of co-axial air flow on the breakup length of a smooth liquid jet (平滑流의 分裂길이에 미치는 同軸氣流의 영향)

  • 김덕줄;이충원
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.12 no.6
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    • pp.1390-1398
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    • 1988
  • The purpose of this study was experimentally to investigate the disintegration process and disintegration mechanism when co-axial air flows vertically for the longest smooth liquid jet. These were affected by liquid velocity, air velocity, air-to-liquid diameter ratio, nozzle shape, and air-liquid contacting position. That is, this process of disintegration of the liquid jet was similar to that occurred when liquid pressure was increased. At Reynolds number of 10, 000 and below, the changes in the breakup length represent different tendency according to liquid flow rate. The influence of air flow on the disintegration of liquid jet was different according to air-to-liquid diameter ratio, air orifice diameter, nozzle shape and contacting position of liquid and air. In particular, when the tip of liquid nozzle was inside the air orifice, the effect of air flow was the larger than outside the air orifice. The effect of liquid mass flow rate on the change rate of the breakup length was also different.

Method and characteristics of liquid atomization (액체 미립화의 방법과 특징)

  • 이충원
    • Journal of the korean Society of Automotive Engineers
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    • v.5 no.4
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    • pp.10-16
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    • 1983
  • 액체의 미립화는 기계산업분야 뿐만 아니라, 농약살포, 화학 공학의 분무건조, 반응의 촉진, 분 체제조, 식품공업 등 폭넓게 이용되며 또한 각분야에서 그 필요성이 강조되고 있다. 특히 기계 산업분야에서는 액체연료의 분무연소(boiler, gas turbine, 자동차용engine등) 원자로 노심의 spray cooling, spray drying, spray painting 등 그 이용도는 날로 증가되는 추세에 있다. 액체를 미 립화하는 이유는 각각의 분야나 사용하는 목적에 따라 다르지만, 대별하면 다음과 같다. (1) 액체의 단위 체적당 표면적을 증대시키기 위하여 (2) 직경이 작은 입자의 필요성 (3) 균일한 입경의 액적군을 얻기 위하여 등을 들 수 있다. 액체의 미립화에 대한 요구는 산업의 발당, 대기오염, 생energy 등의 문제가 중요시됨에 따라 다양화되고 있다. 따라서 응용면에서는 atomizer의 성능개선과 설계법, 새로운 미립화방법, 상업에의 분무이용기술, 분무계측법 등의 개발이 필요하게 된다. 액체미립화에서 취급하는 사항은 그 내용에 따라 다음과 같이 분류된다. (1) 액체의 미립화기구 : 기액계면의 불안정성과 분열기구에 관한 것으로, 액체형상으로써 액주, 액막 및 액적으로 나눌 수 있다. (2) 액체의 미립화 방법과 특성 : energy의 종유와 부가방식에 따랄 나누어진다. (3) 합체, 분산, 증발 등 분무의 운동이나 열적거동 (4) 분무입경이나 운동의 계측법과 특성도시 (5) 액체미립화의 각종응용 본보에서는 상기의 각 항목중, 특히 액체의 미립화방법과 분무특성에 대해서만 말하기로 한다.

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A Study of Mode of Action of Fluazifop-butyl- II. Fluazifop-butyl Effect on Cell Division, Cell Enlargement, and Protein Synthesis in Oat(Avena sativa L.) Roots (Fluazifop-butyl의 제초기구(除草機構)에 관한 연구(硏究)- 제2보(第II報) Fluazifop-butyl이 귀리뿌리의 세포분열(細胞分裂), 세포신장(細胞伸張) 및 단백질합성(蛋白質合成)에 미치는 영향(影響))

  • Kim, Jae-Cheol
    • Korean Journal of Weed Science
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    • v.6 no.2
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    • pp.168-173
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    • 1986
  • The effects of varying concentrations and duration of fluazifop-butyl [(${\pm}$)-butyl [2- [4- [(5-(trifluoro methyl)-2-pyridinyl] oxy] phenoxy] propanate] treatment on cell division, cell enlargement, and protein synthesis were studied. Oat (Avena staiva L.) were treated from 0 to 48 hr with concentration ranging from $1{\times}10^{-6}M$ to $1{\times}10^{-3}M$ of fluazifop-butyl in the cell division study. There was a significant reduction in the mitotic indices of oat roots treated with $1{\times}10^{-4}M$ after 6 hr. After 18 hr treatment, All herbicide treatment inhibited cell division significantly. After 24 hr treatment almost 100% inhibition of cell division occurred at $1{\times}10^{-4}M$ to $1{\times}10^{-3}M$ while 20% inhibition of cell division occurred at $1{\times}10^{-6}M$ concentration at same exposure period. The greatest inhibition of cell division occurred between 0 to 18 hr. The avena coleoptile straight- growth test were used to determine the influence of fluazifop-butyl on eoleoptile growth. Significant inhibition of elongation of oat coleoptiles were observed at $1{\times}10^{-7}M$ to $1{\times}10^{-3}M$ after 24 hr incubation. Protein incorporation study showed that the $1{\times}10^{-4}M$ of fluazifop-butyl caused 60% inhibition of protein synthesis. It was concluded that the growth of inhibition of plants caused by fluazifop-butyl results from inhibition of cell division, cell enlargement, and protein synthesis.

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Breakup Characteristics in Plain Jet Air Blast Atomizer(I)-Jet Breakup and Internal Flow- (2유체 분무노즐의 분열특성(I)-액주분열 및 내부유동-)

  • Kim, Hyeok-Ju;Lee, Chung-Won
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.21 no.8
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    • pp.1009-1023
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    • 1997
  • The breakup length of a liquid jet with flowrate, formed by releasing through a nozzle of circular cross-section into the atmosphere, was experimented and studied for 3 liquid nozzles of varying diameters. The experimental result was analyzed using the existing theoretical equation for predicting the breakup length. It was found that the breakup length of liquid jet depends on the velocity, and the breakup length increases with increasing of the liquid nozzle diameter. Also, the variation range of the breakup length for the same flowrate of liquid increased rapidly as velocity was increased for laminar flow, but in the turbulent flow region, it leveled off in the range of approximately 0.55-0.7 of the mean breakup length. Furthermore, when the longest smooth liquid jet was applied to the co-axial flow air blast atomizer, the effect of air flow on the flow pattern and breakup length was studied for 6 glass nozzles of different lengths and diameters. It was found that depending on the diameter of the mixing tube and liquid jet, it was possible to observe a wide range of flow patterns, such as liquid jet through flow, partial annular flow and annular flow. The liquid jet breakup length was more sensitive to the change in the length rather than the diameter of the mixing tube. As the length of the mixing tube shortens, the breakup length also shortens rapidly.

Experimental Investigation on the Breakup Characteristics of Various Fuels in air Cross-flow Condition (연료 물성에 따른 횡단 유동장 내의 액적 분열 특성에 관한 실험적 연구)

  • Kim, Sa-Yop;Lee, Keun-Hee;Lee, Chang-Sik
    • Journal of ILASS-Korea
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    • v.12 no.3
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    • pp.160-165
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    • 2007
  • In this study, the breakup characteristics of mono disperse droplets were studied with various fuels, ethanol, diesel fuel, biodiesel fuel extracted from soybean oil, and pure water. In order to investigate the droplet behavior in air cross-flow conditions, the experimental equipment was composed of a droplet generator with an air nozzle, and a high-magnification photo detecting system. Droplets produced by the droplet generator were injected into the air stream flowing normal to a direction of liquid drop jet. Digital images of the droplet behavior in air flow field were recorded by controlling the air flow rate. From the inspections, droplet breakup mechanism is primarily classified into the two kinds of stage, first breakup stage and second breakup stage. At the first breakup stage, droplet deformation rate seems to be affected by the force induced by the surface tension and the viscosity. On the other hand, at the second breakup stage, droplet is broken up mainly induced by the surface tension, so the breakup transition can be divided by the regular Weber number.

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An experimental study on mechanism for the disintegration of liquid film surface waves by a parallel air flow (평행공기류에 의한 액막류 표면파의 분열기구에 관한 실험적 연구)

  • 이규영;양옥용
    • Journal of the korean Society of Automotive Engineers
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    • v.14 no.6
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    • pp.81-90
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    • 1992
  • This paper deals with an experimental study on the initial condition of liquid film surface waves disintegration and investigation on the behavior of liquid film surface waves formed by the high speed air flow on the solid plane surface. The authors conducted the qualitative and quantitative study to in vestigate the liquid film flow phenomena, the liquid film disintegration mechanism, and droplet formation process with breaking the liquid film surface wave. The newly devised transparent rectangular test section which has semi-two-dimensional flow at the center of the bottom was introduced to perform the experimental study, and it can generate the uniform thickness liquid film at the bottom. The strobo streak camera was used to obtain the instantaneously transformed photographs. The electronic measuring device was also used to measure the liquid film thickness variation in order to perform the easy and effective analysis of complex flow phenomena in the air-water cocurrent flow.

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An effect of initial disturbance on the breakup mechanism of liquid jet (초기교란이 액주의 분열기구에 미치는 영향)

  • Seok, J.K.;Park, Y.K.;Lee, C.W.
    • Journal of ILASS-Korea
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    • v.3 no.2
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    • pp.34-41
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    • 1998
  • The present experimental study investigates the effect of an initial disturbance on the breakup mechanism of a liquid column. With varying the maginitude of the inital disturbance, we measure the surface wave of liquid column with adopting laser shadow method and analyze the growth rate of liquid column and breakup frequency. The experimental results show that thebreakup characteristics of liquid column is significantly influenced by the frequency of the initial disturbance. We concluded that the most uniform droplet occurs when the frequency of initial disturbance coincides with the natural frequency of the liquid column.

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