• Title/Summary/Keyword: 마이크로 유동학

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마이크로 및 나노 유동학

  • 강인석;임도진
    • Journal of the KSME
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    • v.44 no.10
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    • pp.50-56
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    • 2004
  • 이 글에서 먼저 microfluidics에 관련된 유동제어 기술을 먼저 살펴보고 microfluidic와 nanofluidics의 차이점을 살펴본 후 nanofluidic에 대해 다루기로 한다.

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Experimental Study on Characteristics of Micro-Supersonic Jet Flows (마이크로 초음속 제트유동 특성에 관한 실험적 연구)

  • Kim, Jong-Hun;Bang, Jin-Young;Lee, Yeol
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.36 no.8
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    • pp.774-779
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    • 2008
  • An experimental study on the micro-supersonic jet flow fields has been carried out. A sonic nozzle of 440 ${\mu}m$-exit diameter and a Laval nozzle of 800 ${\mu}m$ exit diameter with the nozzle exit Mach number 2.0 were fabricated by stretching a micro Pyrex glass tube for the present experiments. Schlieren flow visualization and Pitot pressure distribution of the jet flow field were obtained. Representative characteristics of the jet flow fields such as, supersonic length, jet core length, similarity of the velocity field, and jet spreading rates, have been observed. All the results were compared to previous observations of larger supersonic jets of higher Reynolds numbers, and it was found that overall characteristics of the micro supersonic jet are qualitatively similar as those of the higher Reynolds number jets, except the jet core length and the jet spreading rate.

Micro-PIV Analysis of Electro-osmotic Flow inside Microchannels (마이크로 채널 내부 전기삼투 유동에 대한 PIV유동 해석)

  • Kim Yang-Min;Lee Sang-Joon
    • Journal of the Korean Society of Visualization
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    • v.1 no.2
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    • pp.47-51
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    • 2003
  • Microfluidic chips such as lab-on-a-chip (LOC) include micro-channels for sample delivery, mixing, reaction, and separation. Pressure driven flow or electro-osmotic flow (EOF) has been usually employed to deliver bio-samples. Having some advantages of easy control, the flow characteristics of EOF in microchannels should be fully understood to effectively control the electro-osmotic pump for bio-sam-pie delivery. In this study, a micro PIV system with an epifluorescence inverted microscope and a cooled CCD was used to measure velocity fields of EOF in a glass microchannel and a PDMS microchannel. The EOF velocity fields were changed with respect to electric charge of seeding particles and microchannel materials used. The EOF has nearly uniform velocity distribution inside the microchannel when pressure gradient effect is negligible. The mean streamwise velocity is nearly proportional to the applied electric field. Glass microchannels give better repeatability in PIV results, compared with PDMS microchannels which are easy to fabricate and more suitable for PIV experiments.

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Design and Evaluation of a Uniform Flow Microreactor (균일 유동 마이크로 반응기의 설계와 검증)

  • Park, Ji-Min;Yi, Seung-Jae;Kim, Kyung-Chun
    • Journal of the Korean Society of Visualization
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    • v.8 no.3
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    • pp.29-34
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    • 2010
  • This paper proposes a design method to provide uniform flow in a microreactor. Uniform momentum approach is adopted with 10 pillars before and after the chamber having a different slope inlet channel. The slope and number of pillars are two factors to make a uniform flow in the microreactor, covering the hexagonal gold layer. The CFD analysis about the designed microreactor is carried out and the velocity vector field measurements are made in the fabricated microreactor by micro PIV technique. The uniformity of microreactor flow was confirmed by both numerical simulation and experimental results.

PIV Measurements of the Pressure Driven Flow Inside a T-Shaped Microchannel Junction (T헝 마이크로채널 연결부 압력구동 유동의 PIV계측)

  • Choi Jayho;Lee In-Seop
    • Journal of the Korean Society of Visualization
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    • v.1 no.1
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    • pp.75-81
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    • 2003
  • A custom micro-PIV optics assembly has been used to measure the flow fold inside a T-junction of a microchannel. The micro-PIV system consists of microscope objectives of various magnifications, a dichroic cube, and an 8-bit CCD camera. Fluorescent particles of diameters 620 nm have been used with a Nd:YAG laser and color filters. A programmable syringe pump with Teflon tubings were used to inject particle-seeded distilled water into the channel at flow rates of 2.0, 4.0, 6.0 mL/hr. The micro-channels are fabricated with PDMS with a silicon mold, then O$_{2}$ -ion bonded onto a slide glass. Results show differences in flow characteristics and resolution according to fluid injection rates, and magnifications, respectively. The results include PIV data with vector-to-vector distances of 2 $\mu$m with 32 pixel-square interrogation windows at 50$\%$ overlap.

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Efficiency Analysis of Thermal Transpiration According to Knudsen Number for Application to Micro-propulsion System (마이크로 추진장치에 적용을 위한 누센수에 따른 열적발산원리의 효율분석)

  • Jung, Sung-Chul;Huh, Hwan-Il
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.36 no.5
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    • pp.483-490
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    • 2008
  • Minimization of nozzle induces many flow losses in micro-propulsion system. In this study, we studied about thermal transpiration based micro propulsion system to overcome these losses. Thermal transpiration device(Knudsen pump) having no moving parts can self-pump the gaseous propellant by temperature gradient only (cold to hot). We designed, fabricated the Knudsen pump and analyzed pressure gradient efficiency of membrane according to Knudsen number under vacuum condition. Experimental results showed that thick membranes are more effective than thin membranes in transition flow regime, and pressure gradient efficiency according to Knudsen number is increased to maximum 82% apart from membrane thickness in free molecular regime.

Visualization of Electro-osmotic Flow Instability in a T-shape Microchannel (T자형 마이크로 채널 내부 전기삼투 유동의 불안정성 가시화)

  • Han, Su-Dong;Lee, Sang-Joon
    • Journal of the Korean Society of Visualization
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    • v.3 no.2
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    • pp.45-50
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    • 2005
  • Electro-osmotic flow (EOF) instability in a microchannel has been experimentally investigated using a micro-PIV system. The micro-PIV system consisting of a two-head Nd:Yag laser and cooled CCD camera was used to measure instantaneous velocity fields and vorticity contours of the EOF instability in a T-shape glass microchannel. The electrokinetic flow instability occurs in the presence of electric conductivity gradients. Charge accumulation at the interface of conductivity gradients leads to electric body forces, driving the coupled flow and electric field into an unstable dynamics. The threshold electric field above which the flow becomes unstable and rapid mixing occurs is about 1000V/cm. As the electric field increases, the flow pattern becomes unstable and vortical motion is enhanced. This kind of instability is a key factor limiting the robust performance of complex electrokinetic bio-analytical devices, but can also be used for rapid mixing and effective flow control fer micro-scale bio-chips.

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An Experimental Study on the Convection heat Transfer of Al-Mg/water Micro Fluid in a Circular Tube with Swirl (선회유동장에서 Al-Mg/물 마이크로 유동의 대류 열전달에 대한 실험적 연구)

  • Chang, Tae-Hyun;Kim, Chi-Woon;Kil, Sang-Cheol;Lee, Chang-Hoan
    • Journal of the Korean Society of Visualization
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    • v.10 no.3
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    • pp.16-20
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    • 2012
  • In the past decades, extensive studies on convection heat transfer on internal flow have been conducted by using high specific surface area, by increasing heat transfer coefficient and swirl flow, and by improving the transport properties. In this study, we applied a tangential slot swirl generator to improve heat transfer in a horizontal circular copper tube. The Al-Mg particles (approximately $100{\mu}m$ to $130{\mu}m$) were employed for this experimental work. The copper tube was heated uniformly by winding a heating coil with a resistance of 9ohm per meter for heat transfer. Using Al-Mg particles, experiments were performed in the Reynolds number range of 5,000 to 13,130, with and without swirl. Experimental data transfers or comparisons between Nusselt numbers with and without swirl along the test tube and Reynolds numbers are presented. The Nusselt number is improved by increasing Reynolds numbers or swirl intensities along the test tube.