• Title/Summary/Keyword: Microchannel flow

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Analysis of Capillary Flow in Open-Top Rectangular Microchannel (상판이 없는 직사각형 단면의 미세채널에서 모세관 유동 분석)

  • Park, Eun-Jung;Cho, Ji-Yong;Kim, Jeong-Chul;Hur, Dae-Sung;Chung, Chan-Il;Kim, Jung-Kyung
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.34 no.1
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    • pp.77-82
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    • 2010
  • Our study aims to understand the flow of liquid in an open-top rectangular microchannel that can be used in micro total analysis systems ($\mu$-TAS) because it has advantages in terms of light transmission and energy efficiency. We measured the liquid velocity using particle tracking technique and conducted a simulation with computational fluid dynamics by altering the area of channel cross section and channel length for the capillary-driven flow in the open-top rectangular microchannel. When liquid water drops to an entrance of the fabricated microchannel with a height of 20 μm and a width of 20 ${\mu}m$, it flows along the microchannel by only capillary force. In the wetting behavior of the liquid, important parameters of this flow are channel size, contact angle and liquid properties such as surface tension and viscosity, which are used to control the flow of liquid in the microchannel.

Stokes Flow Through a Microchannel with Projections of Constant Spacing (일정 간격의 돌출부를 갖는 마이크로채널 내의 스톡스 유동 해석)

  • Son, JeongSu;Jeong, Jae-Tack
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.39 no.4
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    • pp.335-341
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    • 2015
  • In this study, we analyzed a two-dimensional Stokes flow through a microchannel containing projections with constant spacing attached to each wall. The projections on the top and bottom walls were semi-circular in shape, with in-phase locations. By considering the periodicity and symmetry of the flow, the eigenfunction expansion and least squared error method were applied to determine the stream function and pressure distribution. For some typical radius and spacing values, the streamline patterns and pressure distributions in the flow field are shown, and the shear stress distributions on the boundary walls are plotted. In addition, the average pressure gradients in the microchannel are also calculated and shown with the radius and spacing of the projections. In particular, the results for the case of extremely small gaps between the projections on the top and bottom walls are in good agreement with the lubrication results.

Flow Distribution and Heat Transfer Characteristic of the Microchannel Waterblock with Different Shape of Inlet (미세채널 워터블록의 유입부 형상에 따른 유량분배 및 열유동 특성)

  • Choi, Mi-Jin;Kwon, Oh-Kyung;Yun, Jae-Ho
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.21 no.7
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    • pp.386-393
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    • 2009
  • The present study has been studied on a thermal and flow characteristic of the microchannel waterblock with flow distributions in each channels. Results of a numerical analysis using the CFX-11 are compared with results of an experiment. Numerical analysis and experiment are conducted under an input power of 150 W, inlet temperature of $20^{\circ}C$ and mass flow rates of $0.7{\sim}2.0$ kg/min. Base temperature and pressure drop are investigated with standard deviations of mass flow rates in each channels of samples. The flow distribution and j/f factor of the sample 4 is increased by about 65.7% and 42.6%, compared to that of the reference model sample 3.

Micro PIV measurements of two-fluid flows in a microchannel (Micro-PIV 기법을 이용한 미세유로 내 두 유체 유동 측정)

  • Sung Hyung Jin;Kim Byoung Jae;Liu Ying Zheng
    • 한국가시화정보학회:학술대회논문집
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    • 2004.11a
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    • pp.90-93
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    • 2004
  • Micro PIV was applied to measure velocity profiles of two-fluid flows in a microchannel. In this work, the two-fluid flow of two glycerol-water mixtures was measured for three cases $(\phi=0\;and\;\phi=0.2;\;\phi=0.1\;and\;\phi=0.5;\;\phi=0\;and\;\phi=0.6)$. The flow rates of two fluids were the same. The experimental velocity profiles agreed well with numerical simulations. However, a slight deviation was found in the fluid with low concentration. Rather than the effects of the varying refractive indices inside the channel, the high velocity gradient effect was thought as the main source of the deviation.

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Heat Transfer and Fluid Flow Evaluation of Microchannel Waterblock with Pass Variations (패스변화에 따른 워터블록의 열전달 및 유동특성 평가)

  • Choi, Jin-Tae;Kwon, Oh-Kyung;Choi, Mi-Jin;Yun, Jae-Ho;Kim, Yong-Chan
    • Proceedings of the SAREK Conference
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    • 2009.06a
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    • pp.1135-1140
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    • 2009
  • The present study has been studied on a thermal and flow characteristic of the microchannel waterblock with pass variations in 8 samples. Results of a numerical analysis using the CFX-11 were compared with results of an experiment. Numerical analysis and experiment were conducted under an input power of 150 W, inlet temperature of $35^{\circ}C$ and mass flow rates of $0.7{\sim}2.0\;kg/min$. The numerical results showed reasonably good agreement with the experimental results within about $3{\sim}5%$. Also, the numerical results showed that the sample 2 types with the 2 pass gave better performance than the sample 1 types with the 1 pass from the viewpoints of heat transfer and pressure drop.

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The Heat Transfer and Pressure Drop Characteristics on Microchannel PCHE with various Configurations (채널 형상에 따른 마이크로채널 PCHE의 열전달 및 압력강하 특성)

  • Kim, Yoon-Ho;Moon, Jung-Eun;Lee, Kyu-Jung
    • Proceedings of the SAREK Conference
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    • 2008.11a
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    • pp.215-220
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    • 2008
  • A microchannel PCHE is manufactured by the two technologies of micro photo-etching and diffusion bonding. In this paper, heat transfer and pressure drop characteristics by applying various configuration for the flow channel in the microchannel PCHE is experimentally investigated. The flow channel configurations are designed three types such as straight, wavy and offset strip channels. The performance experiment of each configuration is performed for Reynolds numbers in ranges of $100{\sim}700$ under various flow conditions for the hot side and the Reynolds number of cold side is fixed at 350. The inlet temperatures of the hot side and cold side are conducted as $40^{\circ}C$ and $20^{\circ}C$, respectively. The heat transfer performance of wavy channel, which was similar to that of offset strip channel, was much higher than that of straight channel. The effectiveness of wavy channel and offset strip channel was evaluated as about $0.5{\sim}0.9$. The pressure drop of wavy channel was highest among configurations and that of offset strip channel was lower than that of straight channel because the round curved surface of each strip edge was reduced the pressure loss.

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Boiling Heat Transfer Characteristics of $CO_2$ in Horizontal Smooth Microchannel (수평 microchannel의 $CO_2$ 비등열전달)

  • Choi, Kwang-Il;Ardiyansyah, Ardiyansyah;Oh, Jong-Taek
    • Proceedings of the SAREK Conference
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    • 2007.11a
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    • pp.241-246
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    • 2007
  • The present paper dealt with an experimental study of boiling heat transfer characteristics of $CO_2$. Heat transfer coefficients of the refrigerant flow inside horizontal smooth microchannel were obtained with inner tube diameter of 0.3mm and length of 300mm. The direct electric heating method was applied for supplying the heat uniformly to the refrigerant. The experiments were conducted with $CO_2$ purity of 99.99%, at saturation temperature of $10^{\circ}C$, mass flux ranges of $300{\sim}900\;kg/m^2s$, and heat flux ranges of $15{\sim}45\;kW/m^2$. While heat transfer coefficient increased with the increase of heat flux in the low quality region, the heat transfer coefficient decreased with the increase of quality in the high quality region. The heat transfer coefficients were compared with seven existing correlations with the Gungor-Winterton's(1986) correlation gave the best prediction. A new corelation to predict the two-phase flow heat transfer coefficient was developed based on the Chen(1966) correlation. The new correlation predicted the experimental data well with a mean deviation of 9.69% and average deviation of -3.03%.

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Flow Rate Changes in the Heterogeneous Rectangular Microchannels with Different Hydrophilicity for the PDMS Bottom Surface (PDMS 표면특성에 따른 비균일계 마이크로채널의 유속 변화)

  • Noh, Soon-Young;Lee, Hyo-Song;Kim, Ki-Ho;Choi, Jae-Ho;Yu, Jae-Keun;Yoon, Soo-Kyung;Rhee, Young-Woo
    • Clean Technology
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    • v.13 no.3
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    • pp.195-200
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    • 2007
  • This study investigated the flow rate changes of the heterogeneous rectangular microchannels which have different hydrophilic property on the bottom surface. The heterogeneous rectangular microchannel has three native PDMS (poly-dimethyl siloxane) surfaces which were patterned by the soft lithography. PDMS bottom surface was treated by the argon plasma and coated by the allyl alcohol (99%). The channel length was 10, 20 and 30 mm and the channel width was 100, 200 and $300\;{\mu}m$, respectively. Several external voltages were applied to make the fluid flow by the electroosmosis in the microchannel. For the same electric field strength and hydrophilicity of the bottom surface, the flow rate is almost same. This result is matched to the theoretical expectation and confirms that the experimental system is reliable. With increasing the channel width, the flow rate increased for the same hydrophilicity of the bottom surface. The flow rate of the microchannel of higher hydrophilicity was larger than that of the microchannel of lower hydrophilicity. This result implies that the hydrophilicity change of the bottom surface could be applied to control the flow rate in the microchannel.

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A Study on Fluid Flow Characteristic In a Microchannel (미세 유로에서의 유동 특성에 관한 연구)

  • Kim, Hyung-Woo;Oh, Jae-Geun;Jeong, Si-Young;Choi, Bum-Kyoo
    • Proceedings of the KIEE Conference
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    • 1999.07g
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    • pp.3282-3285
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    • 1999
  • Fluid characteristics at microscale were tried to be solved in this paper by showing how they deviate with conventional flow governing equations. (e.g. Navier-Stokes Equation) In earlier studies, this deviation phenomena was caused because of omitting no slip flow condition, micropolar effect and EDL(Electric Double Layer)effect of fluid which are usually negligible at macroscaled phenomena. The characteristics of fluid flow were tried to be studied by measuring pressure difference of specified length of the channels using the almost squared micromachined channels. By acquiring pressure difference, we could drive different values (viscosity, flow velocity. etc) from it and these data will be compared with macroscaled flow characteristics. As making microchannel is not easy work and that our knowledge is at mere stage, we had to fail to make it in this time. The hardest thing in this work is to make a hole which is directly connected with channel. The more efficient and easy way of making microchannel is proposed in this paper.

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Fabrication of the Microchannel Integrated with the Inner Sensors for Accurate Measuring Fluid Temperature (유체의 정확한 온도 측정을 위하여 내부 센서를 집적한 마이크로채널 제작)

  • Park, Ho-Jun;Im, Geun-Bae;Son, Sang-Yeong;Song, In-Seop;Park, Jeong-Ho
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.51 no.9
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    • pp.449-454
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    • 2002
  • A rectangular straight microchannel, integrated with the resistance temperature detectors(RTDs) for temperature sensing and a micro-heater for generating the Temperature gradient along the channel, was fabricated. Its dimension is 57${\mu}{\textrm}{m}$(H)$\times$200${\mu}{\textrm}{m}$(W)$\times$48,050${\mu}{\textrm}{m}$(L), and RTDs were placed at the inner-channel wall. Si wafer was used as a substrate. For the fabrication of RTDs, 5300$\AA$ thick Pt/Ti layer was sputtered on a Pyrex glass wafer. Finally, the glass wafer was bonded with Si wafer by anodic bonding, so that the RTDs are located inside the microchannel. Temperature coefficient of resistance(TCR) values of the fabricated Pt-RTDs were 2800~2950ppm$^{\circ}C$ and the variation of TCR value In the range of O~10$0^{\circ}C$ was less than 0.3%. Therefore, it was proved that the fabricated Pt-RTDs without annealing were excellent as temperature sensors. The temperature distribution in the microchannel was investigated as a function of mass flow rate and heating power. The temperature increase rate diminished with decreasing the applied power and increasing the mass flow rate. It was confirmed from the comparison with the simulation results that the temperature measured inside the microchannel is more accurate than measuring the temperature measured at the outer wall. The proposed temperature sensing method and microchannel are expected to be useful in microfluidics researches.