Dissertations / Theses on the topic 'Microchannel Heat Transfer'
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Siu, Billy Chin Pang. "Condensation heat transfer in microchannel /." View abstract or full-text, 2004. http://library.ust.hk/cgi/db/thesis.pl?MECH%202004%20SIU.
Full textIncludes bibliographical references (leaves 43-46). Also available in electronic version. Access restricted to campus users.
Lee, Man. "Forced convection heat transfer in integrated microchannel heat sinks /." View abstract or full-text, 2006. http://library.ust.hk/cgi/db/thesis.pl?MECH%202006%20LEE.
Full textTurgay, Metin Bilgehan. "Effect Of Surface Roughness In Microchannels On Heat Transfer." Master's thesis, METU, 2008. http://etd.lib.metu.edu.tr/upload/12610253/index.pdf.
Full textAl-Waaly, Ahmed. "The effect of heat transfer on temperature measurement and its applications to study microchannel heat sinks." Thesis, University of Glasgow, 2015. http://theses.gla.ac.uk/6781/.
Full textOjada, Ejiro Stephen. "Analysis of mass transfer by jet impingement and study of heat transfer in a trapezoidal microchannel." [Tampa, Fla] : University of South Florida, 2009. http://purl.fcla.edu/usf/dc/et/SFE0003297.
Full textDeterman, Matthew D. "Experimental and Analytical Investigation of Ammonia-Water Desorption in Microchannel Geometries." Thesis, Georgia Institute of Technology, 2005. http://hdl.handle.net/1853/7149.
Full textRastan, Hamidreza. "Investigation of the heat transfer of enhanced additively manufactured minichannel heat exchangers." Thesis, KTH, Skolan för industriell teknik och management (ITM), 2019. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-264278.
Full textGokaltun, Seckin. "Lattice Boltzmann Method for Flow and Heat Transfer in Microgeometries." FIU Digital Commons, 2008. http://digitalcommons.fiu.edu/etd/64.
Full textBakaraju, Omkareshwar Rao. "Heat Transfer in Electroosmotic Flow of Power-Law Fluids in Micro-Channel." Cleveland State University / OhioLINK, 2009. http://rave.ohiolink.edu/etdc/view?acc_num=csu1263337731.
Full textCetin, Barbaros. "Analysis Of Single Phase Convective Heat Transfer In Microtubes And Microchannels." Master's thesis, METU, 2005. http://etd.lib.metu.edu.tr/upload/12605820/index.pdf.
Full textBard, Ari. "Modeling and Predicting Heat Transfer Coefficients for Flow Boiling in Microchannels." Case Western Reserve University School of Graduate Studies / OhioLINK, 2021. http://rave.ohiolink.edu/etdc/view?acc_num=case1619091352188123.
Full textMartínez, Ballester Santiago. "NUMERICAL MODEL FOR MICROCHANNEL CONDENSERS AND GAS COOLERS WITH AN IMPROVED AIR-SIDE APPROACH." Doctoral thesis, Universitat Politècnica de València, 2012. http://hdl.handle.net/10251/17453.
Full textMartínez Ballester, S. (2012). NUMERICAL MODEL FOR MICROCHANNEL CONDENSERS AND GAS COOLERS WITH AN IMPROVED AIR-SIDE APPROACH [Tesis doctoral no publicada]. Universitat Politècnica de València. https://doi.org/10.4995/Thesis/10251/17453
Palancia
Stocks, Marc Darren. "Geometric optimisation of heat transfer in channels using Newtonian and non-Newtonian fluids." Diss., University of Pretoria, 2012. http://hdl.handle.net/2263/33348.
Full textDissertation (MEng)--University of Pretoria, 2012.
gm2014
Mechanical and Aeronautical Engineering
unrestricted
Fronk, Brian Matthew. "Coupled heat and mass transfer during condensation of high-temperature-glide zeotropic mixtures in small diameter channels." Diss., Georgia Institute of Technology, 2014. http://hdl.handle.net/1853/52265.
Full textBroderick, Spencer L. "Thermally Developing Electro-Osmotic Convection in Circular Microchannels." BYU ScholarsArchive, 2004. https://scholarsarchive.byu.edu/etd/232.
Full textKorniliou, Sofia. "Experimental study on local heat transfer coefficients and the effect of aspect ratio on flow boiling in a microchannel." Thesis, University of Edinburgh, 2018. http://hdl.handle.net/1842/31080.
Full textMlcak, Justin Dale. "Simulation of three-dimensional laminar flow and heat transfer in an array of parallel microchannels." [College Station, Tex. : Texas A&M University, 2007. http://hdl.handle.net/1969.1/ETD-TAMU-1671.
Full textWang, Wei-Wen William. "Condensation and single-phase heat transfer coefficient and flow regime visualization in microchannel tubes for HFC-134A /." The Ohio State University, 1999. http://rave.ohiolink.edu/etdc/view?acc_num=osu1488192119266647.
Full textBustamante, John Gabriel. "Falling-film evaporation over horizontal rectangular tubes." Diss., Georgia Institute of Technology, 2014. http://hdl.handle.net/1853/52296.
Full textHu, Xinqun. "Design of a microchannel reactor for gas phase heterogeneous reactions : enhanced mass and heat transfer for process intensification." Thesis, University of Sheffield, 2001. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.246984.
Full textGozukara, Arif Cem. "Analysis Of Single Phase Convective Heat Transfer In Microchannels With Variable Thermal Conductivity And Variable Viscosity." Master's thesis, METU, 2010. http://etd.lib.metu.edu.tr/upload/2/12611549/index.pdf.
Full textGoktolga, Mustafa Ugur. "Simulation Of Conjugate Heat Transfer Problems Using Least Squares Finite Element Method." Master's thesis, METU, 2012. http://etd.lib.metu.edu.tr/upload/12614787/index.pdf.
Full textquadrilateral and triangular elements for two dimensional problems, hexagonal and tetrahedron elements for three dimensional problems were tried. However, since only the quadrilateral and hexagonal elements gave satisfactory results, they were used in all the above mentioned simulations.
Martin, Callizo Claudi. "Flow Boiling Heat Transfer in Single Vertical Channels of Small Diameter." Doctoral thesis, KTH, Tillämpad termodynamik och kylteknik, 2010. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-25797.
Full textQC 20101101
Shinde, Pradeep R. "Investigation of Low Reynolds Number Flow and Heat Transfer of Louvered Surfaces." FIU Digital Commons, 2016. http://digitalcommons.fiu.edu/etd/3038.
Full textCowley, Adam M. "Hydrodynamic and Thermal Effects of Sub-critical Heating on Superhydrophobic Surfaces and Microchannels." BYU ScholarsArchive, 2017. https://scholarsarchive.byu.edu/etd/6572.
Full textCelik, Sitki Berat. "Analysis Of Single Phase Fluid Flow And Heat Transfer In Slip Flow Regime By Parallel Implementation Of Lattice Boltzmann Method On Gpus." Master's thesis, METU, 2012. http://etd.lib.metu.edu.tr/upload/12614943/index.pdf.
Full textOwhaib, Wahib. "Experimental Heat Transfer, pressure drop, and Flow Visualization of R-134a in Vertical Mini/Micro Tubes." Doctoral thesis, KTH, Tillämpad termodynamik och kylteknik, 2007. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-4299.
Full textQC 20100812
Nascimento, Francisco Júlio do. "Estudo teórico-experimental da transferência de calor e da perda de pressão em um dissipador de calor baseado em microcanais." Universidade de São Paulo, 2012. http://www.teses.usp.br/teses/disponiveis/18/18147/tde-14082012-113947/.
Full textThis study presents a theoretical and experimental investigation on single and two-phase flows in a microchannel based heat sink. Multi-microchannel heat sinks are able of dissipating extremely high heat fluxes under confined conditions. Such characteristics have attracted the attention of academia and industry and actually several studies are being carried out in order to evaluate and optimize such devices. Initially, an extensive investigation of the literature concerning convective boiling in micro-scale channels was performed. This literature review covers transitional criteria between micro- and macro-scale flow boiling, two phase flow patterns, heat transfer coefficient and pressure drop during convective boiling. Special attention was given to studies concerning microchannels based heat sinks. Based on this investigation, an experimental facility was built for performing heat transfer and pressure drop measurements during single-phase flow and flow boiling in microchannel based heat sinks. For this study, a microchannel based heat sink was also manufactured. The heat sink contains 50 rectangular parallel microchannels, 15 mm long, 100 µm wide by 500 µm deep and separated by 200 µm walls. Experiments were performed for R134a, mass velocity of 400-1500 kg/m²s, maximum vapor quality of 0,35 and heat fluxes up to 310 kW/m². The database obtained in the present study was compared against pressure drop and heat transfer coefficient prediction methods from the literature. It was found that no one method is accurate in predicting heat sink pressure drop while heat transfer coefficient results were accurately predicted by the 3-zone model proposed by Thome et al. (2004).
Leão, Hugo Leonardo Souza Lara. "Análise experimental dos efeitos do fluido e da orientação do escoamento no desempenho de dissipadores de calor baseados na ebulição convectiva em microcanais." Universidade de São Paulo, 2014. http://www.teses.usp.br/teses/disponiveis/18/18147/tde-19082014-102054/.
Full textThis study presents an experimental investigation on the effect of the fluid and the footprint orientation on the performance of a heat spreader based on flow boiling inside micro-scale channels. This heat spreader is used in an electronics cooling application with high-power density. Initially an extensive investigation of the literature concerning single-phase and two-phase flow inside a single microchannels and multi-microchannels was performed. In this literature review the leading predictive methods for heat transfer coefficient and pressure drop are described. The experimental study was carried out in the apparatus developed by Do Nascimento (2012). The heat sink evaluated in the present study is comprised of fifty parallel rectangular microchannels with cross-sectional dimensions of 100 µm width and of 500 µm depth, and total length of 15 mm. The fins between consecutive microchannels are 200 µm thick. Experimental tests were performed for R245fa, low-pressure fluid used in low pressure refrigeration cycles, and R407C, high-pressure fluid used for heat comfort, saturation temperature of 25 and 31°C, mass velocities from 400 to 1500 kg/m² s, degrees of subcooling of the liquid of 5, 10 and 15°C, outlet vapor quality up to 0.38, heat fluxes up to 350 kW/m², and for the following footprint heat sink orientations: horizontal, vertical with the microchannels aligned horizontally and vertical with upward flow. The results were parametrically analyzed and compared again the predictive methods from literature. Average heat transfer coefficients up to 35 kW/m² °C were obtained. The results for R134a from Do Nascimento (2012) for the same heat sink presented heat transfer coefficients higher than R245fa and R407C. The fluid R407C presented oscillation of the temperature due to thermal instability effects with lower frequency and amplitude lower than R134a, and R245fa. None predictive method provided satisfactory heat transfer coefficient and pressure drop predictions of the experimental data. The Homogeneous model with the viscosity given by Cicchitti et al. (1960) provided the best pressure drop prediction while the heat transfer coefficient was best predicted by Bertsch et al. (2009) and Liu and Winterton (1991). The horizontal orientation of the footprint provided the highest heat transfer coefficients while the vertical footprint orientation with upward flow the lowest pressure drops. Images of the two-phase flow were obtained with a high-speed camera and analyzed.
Tibiriçá, Cristiano Bigonha. "Estudo teórico-experimental da transferência de calor e do fluxo crítico durante a ebulição convectiva no interior de microcanais." Universidade de São Paulo, 2011. http://www.teses.usp.br/teses/disponiveis/18/18147/tde-22092011-161901/.
Full textThis research comprises an experimental and theoretical study on flow boiling heat transfer and critical heat flux inside small diameter tubes based on data obtained in experimental facilities specially designed for this purpose. A broad literature review was carried out and the main methods to predict the heat transfer coefficient, critical heat flux and flow patterns were pointed out. The experimental results were parametrically analyzed and compared against the predictive methods from literature. For the first time, microchannels experimental results obtained by an unique researcher in distinct laboratories were compared and a reasonable agreement was observed. The importance of such a comparison is high-lighted for flow boiling inside microchannels due to the high discrepancies ob-served when results from independent laboratories obtained under similar experimental conditions are compared. Moreover, the experimental results obtained in the present study were used to develop correlations and models for the heat transfer coefficient and heat flux that takes into account the flow patterns observed in microchannels. The heat transfer coefficient and critical heat flux models were developed based on mechanistic approach. In addition, criteria to characterize macro to microchannel transition were proposed based in the occurrence of the stratified flow pattern and the liquid film symmetry under annular flow conditions.
Mala, Gh Mohiuddin. "Heat transfer and fluid flow in microchannels." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 1999. http://www.collectionscanada.ca/obj/s4/f2/dsk1/tape8/PQDD_0005/NQ39562.pdf.
Full textMoore, Bryce Kirk. "Gas-liquid flows in adsorbent microchannels." Thesis, Georgia Institute of Technology, 2013. http://hdl.handle.net/1853/47519.
Full textSu, Qian. "Experimental investigation of condensation heat transfer in microchannels." Thesis, Queen Mary, University of London, 2007. http://qmro.qmul.ac.uk/xmlui/handle/123456789/1588.
Full textBarber, Jacqueline Claire. "Hydrodynamics, heat transfer and flow boiling instabilities in microchannels." Thesis, University of Edinburgh, 2010. http://hdl.handle.net/1842/4000.
Full textIrwansyah, Ridho [Verfasser], Christian J. [Akademischer Betreuer] Kähler, Christian J. [Gutachter] Kähler, and Christian [Gutachter] Cierpka. "On the experimental investigation of the laminar convective heat transfer of Al₂O₃-water nanofluids in a microchannel / Ridho Irwansyah ; Gutachter: Christian J. Kähler, Christian Cierpka ; Akademischer Betreuer: Christian J. Kähler ; Universität der Bundeswehr München, Fakultät für Luft- und Raumfahrttechnik." Neubiberg : Universitätsbibliothek der Universität der Bundeswehr München, 2018. http://d-nb.info/1169088996/34.
Full textAgarwal, Akhil. "Heat Transfer and Pressure Drop During Condensation of Refrigerants in Microchannels." Diss., Georgia Institute of Technology, 2006. http://hdl.handle.net/1853/14129.
Full textKuan, Wai Keat. "Experimental study of flow boiling heat transfer and critical heat flux in microchannels /." Link to online version, 2006. https://ritdml.rit.edu/dspace/handle/1850/1887.
Full textInjeti, Phaninder. "Numerical simulation of steady state and transient heat transfer in microchannels." [Tampa, Fla.] : University of South Florida, 2007. http://purl.fcla.edu/usf/dc/et/SFE0002157.
Full textTu, Kuan-Hsu, and 凃冠旭. "Condensation Heat Transfer Enhancementin Microchannel." Thesis, 2013. http://ndltd.ncl.edu.tw/handle/61905943294136803719.
Full text國立臺灣大學
機械工程學研究所
101
The microchannel evaporator with two-phase heat transfer achieves a high heat transfer coefficient, and low working fluid demands; therefore, is considered to have high potential. Thus, the use of microchannel condenser that uses two-phase heat transfer is seen as a cooling component with very high potential. By making it a porous structure that creates a 3D porous network, resulting in advantages such as large evaporation area, high capillary force, and high permeability, the heat transfer performance of the microchannel condenser is expected to increase significantly. This study used copper to manufacture both the flat-plate microchannel condenser and porous microchannel condenser, with 30 microchannels of width and depth 500μm×155μm; Using water as working fluid, with mass flux range of 65~95 kg/m2 s, for heat transfer performance test. This study first investigates the effect of copper powder size and the structure’s base thickness of a porous microchannel condenser on heat transfer performance, then compares its heat transfer performance, pressure drop, and flow patterns to those of flat-plate microchannel condenser. Comparing experimental results for heat transfer performance to heat transfer correlation of the conventional channel showed that the MAE is still large. With regard to pressure drop, compare with the correlation of microchannel developed recently, it correlated with our result, indicating a certain degree of reliability. For flat-plate microchannel condenser, from flow visualizations of flows, 5 most common types of flow in condensation process can be seen clearly: droplet flow, annular flow, injection flow, slug flow, and bubbly flow. Heat transfer coefficient and pressure drop is positive correlative with increasing mass flux. When mass flux increases, the flow velocity increases, and the liquid-vapor interface shear stress increases, resulting in thinning of the liquid film, and the annular flow region increases; the heat transfer performance was thus enhanced accordingly. Heat transfer coefficient is 23~79kw/m2k. The overall pressure drop was also enhanced due to increased flow rate of the working fluid and elongation of the two-phase region. For porous microchannel condenser, manufacturing parameters such as the base thickness range of 150~300μm and copper powder diameter range of 1~150μm was investigated. Experimental results showed that highest heat transfer coefficient was achieve with base thickness of 150μm and powder diameter of 88μm; heat transfer coefficient is 43~161kw/m2k, on average, the heat transfer coefficient of porous microchannel condenser was increased by 110% compared to that of flat-plate microchannel condenser. The absorption of condensed water build up by a porous microchannel structure allows for the thinning of the condensed liquid film and the annular flow region is more extended, therefore its heat transfer performance is better than that of a regular flat-plate microchannel condenser. Concerning pressure drop, the overall pressure drop is greater than that for flat-plate microchannel condenser, with a greatest enhancement value of 15kpa. To summarize this study, porous microchannel effectively enhance the heat transfer performance of condenser, It is highly potential for the high-power thermal management application.
Huang, Yu Hsiang, and 黃友相. "Laminar Heat Transfer in Microchannel." Thesis, 1999. http://ndltd.ncl.edu.tw/handle/33228770672319143894.
Full textLi, Po-Yen, and 李柏諺. "Condensation Heat Transfer Enhancement by Porous Microchannel." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/28395483904510377861.
Full text國立臺灣大學
機械工程學研究所
100
The microchannel evaporator with two phase heat transfer is considered to be one of the most potential cooling techniques because of its high heat flux, good temperature uniformity and the lesser requirement for coolant flow rate. In recent years, the heat dissipation rate of the high tech products has increased day by day. The traditional single-phase heat exchanger could not efficiently cool down in a limited area, so the microchannel condenser with two phase heat transfer is regarded as a high potential cooling component in the future. The central purpose of the present research is to enhance the condensation heat transfer by utilizing the two pore size distributions of a biporous surface structure. This surface is sintered from the mixture of dendritic copper powders and the pore former, Na2CO3, which formed the different size pores in the microchannel. By changing the volumetric ratio of pore former, it was able to alter the porosity and the numbers of larger pores, further increasing the heat transfer coefficient. During condensation, vapor could go through the larger pores. The smaller pores could absorb the liquid and help to reduce the liquid film thickness. It decreased the heat resistant and increased the heat transfer coefficient. First, a plane surface microchannel system was built as a compared base. The test section of the 30 channels where the width and the depth is 500μm and 155μm, respectively. The test section was made by oxygen-free copper. Water steam is using as working fluid. In the experiment of the plane surface microchannel, the heat transfer coefficient and the pressure drop werw positively related to the increasing mass flux. When increasing the mass flux, the velocity of working fluid becomes faster due to the increasement of wall shear stress. Therefore, it caused the thickness of the liquid film much thinner, decreased the heat resistance and also increased the heat transfer coefficient. Compared with the heat transfer correlation of the conventional channel, the result showed the MAE is quite large. That means there is much room to make progress on the heat transfer correlation of the microchannel. With regard to the pressure drop, comparing with the correlation of microchannel in recent years, it considerably correlated with the results. That shows the result is reliable. For experiment of the biporous surface microchannel, the parameter with copper powder is 61~70 μm diameter and volumetric ratio of Na2CO3 is 30%. Comparing with the plane surface microchannel, the results showed that the heat transfer coefficient is enhanced to 72.9% on average when increased the pressure drop to 28.6% on average. The main reasons of enhancing the heat transfer are high water absorbing capacity and good ability for reducing liquid thickness.
Liu, Bing-Han, and 劉秉翰. "Heat Transfer Enhancement in Porous Microchannel Evaporator." Thesis, 2011. http://ndltd.ncl.edu.tw/handle/25368331614143280375.
Full text國立臺灣大學
機械工程學研究所
99
The microchannels evaporator, which possesses the advantages of high heat transfer coefficient, good temperature uniformity, and small requirement for coolant flow rates, is considered as a potential cooling technology. In recent years, the raising of heat dissipation rate in electrical products becomes an important issue. The heat-transfer enhanced microchannels are suitable for the applications. The porous structure with a large number of nuclear sites as well as the re-entrance cavities is expected to enhance the heat transfer performance in a microstructure. In the present study, porous microchannel evaporators are designed and manufactured. The effects of powder size, thickness of structure, and pore size distribution upon the heat transfer performance are investigated. The comparisons of heat transfer characteristics, pressure drop, pressure instability, and heat transfer enhanced effects between the plane and the porous microchannel evaporator are made. The flow boiling experiments were conducted with a plane and a porous microchannel evaporator using R-134a as coolant. Both microchannels had 62 channels (225μm in width; and 660μm in depth) on copper substrates with one square inch in area. For the plane microchannel evaporators, the results showed that the nucleation boiling and the force convection boiling mechanisms both appeared in microchannels. When the quality in the microchannels was smaller than 0.4, the heat transfer coefficient mainly increased with increasing heat flux and did not vary with the mass flow rate or the quality. This region (quality was under 0.4) was dominated by the nucleation boiling mechanism. On the other hand, when the quality was larger than 0.4, the heat transfer coefficient increased with a increasing mass flux. This region (quality was over 0.4) was dominated by the force convection boiling. The experiment results were substituted into the correlations in which the surface tension force was taken into consideration. The predictions showed a good agreement with experimental data. The critical heat flux (CHF) increased with increasing flow rates. A CHF correlation that incorporates the surface tension force showed an excellent accuracy for the experimental data. Pressure drop were raised by increasing flow rates and heat fluxes. The separation model incorporating surface tension force had a good agreement. The pressure drop oscillation suggested that the presence of instability inside the plane microchannels as well as the maximum amplitude of oscillation were found near the onset of nucleation (ONB). For the porous microchannels evaporator, the experimental results depicted that the heat transfer coefficient reached a peak value at low quality and decreased with a increasing quality. However, the heat transfer coefficient did not vary with the mass flow rate. This was apparently different from the plane microchannels. The heat-transfer behavior dominated by the mass fluxes belongs to the force convection boiling mechanism. In contrast of the plane microchannel evaporator, the heat transfer coefficient in the porous microchannels evaporator had an enhancement of 5 times in average. The CHF in porous microchannel evaporator increased with increasing mass fluxes and did not enhanced significantly. Furthermore, the trend of pressure drop in porous microchannel was similar in the plane microchannels. The pressure drop was higher than plane microchannels; however, the maximum pressure drop was not over 50%. The amplitude of average pressure drop oscillation near the high heat flux as well as ONB was 1/6 and 1/2 smaller than in the plane microchannels. This result presented that the porous microchannels evaporators provided a stable boiling behavior when the nucleation began. The porous microchannel evaporators were sintered under the following parameters: the powder diameter dp ranged from 1~100μm, thickness of porous structure δ ranged from 150~375μm, and δ/dp ranged from 2~20, respectively. The investigation on the effect of particle size dp as well as thickness δ indicated that the ratio of the thickness to the particle size δ/dp had a significance in the heat transfer performance. This ratio must be properly chosen in order to reach a better heat transfer performance. The better ratio of δ/dp was between 8~12 in our work. Moreever, the pore size distribution dominated the heat transfer behavior. Smaller pore size with a higher heat transfer capacity. The bi-porous structure was better than the mono-porous structure in about 2 times. To conclude the present study, the porous microchannel evaporator is highly potential for the industrial applications.
Chiu, Yi-Shan, and 邱義善. "Investigation of Heat Transfer on Microchannel Evaporator." Thesis, 2007. http://ndltd.ncl.edu.tw/handle/24616800940770022083.
Full text國立臺灣大學
機械工程學研究所
95
Microchannles provide a large heat transfer surface area per unit flow volume. Phase change in microchannel evaporator makes it desirable for three reasons:(1) high critical heat flux (2) high heat transfer coefficient (3) low coolant flow rate. Therefore, they are well suited for high heat flux removal and high temperature uniformity cooling applications. Present research successfully established a reliable microchannel evaporator experimental system to investigate heat transfer behavior in microchannels and enhance heat transfer performance by sintered porous structure. The working liquid used is refrigerant R-134a, operating pressure is 8 bar, and mass flux ranges from 222 to 464kg/m2s. The microchannel evaporator was fabricated from oxygen-free copper, and top platform was cut to form 62 parallel rectangular 225μm×660μm microchannels. The top platform of porous microchannel evaporator was sintered to form 62 parallel rectangular 210μm×660μm microchannels. The thickness of porous surface structure is 96μm, and the porosity is 54%. The average particle size is 30μm. The results reveal that flow boiling pressure drop is primarily affected by mass velocity and heat flux, which increases with increasing mass velocity and heat flux. The predictability of separated flow model is much better than homogeneous equilibrium model on flow boiling pressure drop in microchannel, and the lowest MAE is 10.6%. Flow boiling in microchannel can be classified either as boiling-dominated region or convection-dominated region. In boiling-dominated region, the heat transfer coefficient increases with increasing heat flux. In convection-dominated region, the heat transfer coefficient decreases with decreasing vapor quality. These two region are separated by the peak value of heat transfer coefficient, and this separation will change if mass velocity differs. The heat transfer data closely match with some previous correlations, and the lowest MAE is 13.6%. The critical heat flux is primarily affected by mass velocity, which increases with increasing mass velocity. The CHF data also closely match with some previous correlations, and the lowest MAE is 2.6%. As for heat transfer enhancement, in the same volume flow rate 167 ml/min, the heat transfer coefficient and CHF of porous microchannel evaporator is enhanced by 2-3.8 times and 19-23% respectively.
Li, Wei-ping, and 李偉平. "Heat Transfer Analysis and Channel Designs of Microchannel Heat Sinks." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/96896024583791424982.
Full text國立臺南大學
綠色能源科技研究所碩士班
100
In this thesis, the numerical analysis is performed to examine the possible methods to enhance the heat transfer performance of microchannel heat sink (MCHS) by computational fluid dynamics software. The effects of geometric parameters and nanofluids are discussed in details for the enhancement of heat transfer performance in MCHs. For the design of two-layer MCHS, the effects of geometric parameters such as channel number, channel width ratio, channel aspect ratio, and pumping power on the temperature distribution and thermal resistance are discussed in details. For the design of tapered MCHS, the effects of tapered ratios of height and width the thermal performance are discussed. For the nanofluids, the double-layered MCHS with different particle volume fractions, particle sizes, and pumping powers are presented. Predictions show that the heat transfer performance of the two-layered MCHS can be improved for a system. For the triple-layered MCHS, higher performance is found for a system with lower aspect ratio of the middle layer when the aspect ratio of the bottom layer is fixed. As for the tapered MCHS, the tapered channel in MCHS would affect the flow field and pressure drop. The pressure drop increases with both the tapered ratios in height and width. For fixed pumping power, the effects of tapered channel in width on the thermal performance. With fixed pumping power, the nanofluid MCHSs with lower base fluid viscosity have a more effective heat transfer enhancement, relatively to those of pure fluid MCHSs. Besides, the predicted showed that best thermal performance of MCHS is found for a nanofluid with 1% particle volume fraction.
Tunc, Gokturk. "Convective heat transfer in microchannel gaseous slip flow." Thesis, 2002. http://hdl.handle.net/1911/18142.
Full textChen, Kuei-Yen, and 陳奎延. "Wettability Effect on Microchannel Condenser Heat Transfer Enhancement." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/18284612827192116300.
Full text國立臺灣大學
機械工程學研究所
100
In recent years, the microchannel evaporator with two phase heat transfer, due to its highly heat flux and little requirement for coolant flow rate, is considered as one of potential cooling techniques. When the traditional single phase heat exchanger cannot efficiently cool in a limited area, collocating the microchannel condenser with two phase heat transfer is regarded as a potential cooling component. Because of the highly developed technology, the heat dissipation rate raise in many products. Therefore the microchannel condenser with enhanced heat transfer is more applicale. The hydrophobic surface has wide contact angle, and worse wettbility. In the process of condensation it will form dropwise condensation. The heat transfer coefficient is increased dramatically in the large scale condenser within hydrophobic surface. We assume that it will show the same result in the microchannel condenser. Thus, this research design and manufacture the hydrophobic and hydrophilic microchannel condenser, compare to the heat transfer coefficient and pressure drop with uncoated microchannels condenser. The test section has 30 channels 500μm in width and 155μm in depth using water as working fluid. Using layer-by-layer (LbL) assembly method manufacture the hydrophobic and hydrophilic structure the same geometric dimensions microchannel condenser. In the experiment of the uncoated microchannel, the heat transfer coefficient and pressure drop is positive correlative with the increasing mass flux. Because increasing the mass flux, the velocity becomes faster, along with increasing the wall shear stress. This will make the thickness of the liquid film become much thinner, and reduce the heat resistant, further increase the heat transfer coefficient. Compared with the heat transfer correlation of the conventional channel, the result shows the MAE is still large. Currently, there is still much room to make progress on the heat transfer correlation of the microchannels. With regard to the pressure drop, compare with the correlation of micrchannel developed recently, it correlated with our result and shows that our result is reliable. In coated surface, we use layer-by-layer (LbL) assembly method to change the contact angle between water and copper, to manufacture the hydrophobic and hydrophilic structure. The contact angle of the hydrophilic structure change from 87°to 43°. Also the contact angle of the hydrophobic structure rise up to 135°. Compared with the heat transfer coefficient of the uncoated surface, the hydrophobic microchannels can increase roughly 100% on average, with remarkable difference. The droplet cannot adhere on the hydrophobic surface to cause the dropwise condensation. The mechanism is different from the filmwise condensation. Therefore, the heat transfer coefficient is much higher. When the mass flux is small, the heat transfer coefficient doesn’t increase remarkably. Because the velocity is slower, the liquid film is easy to form. Therefore, the mechanism that dropwise condensation could increase the heat transfer coefficient cannot be observed within the small mass flux in this experiment. As increasing the mass flux, the velocity is so fast that is not easy to form the liquid film. This will make the heat transfer coefficient increase remarkably. For the pressure drop, the contact angle of the hydrophilic structure is smaller, and it can extend liquid, making the flow easier. In this experiment the pressure drop decrease about 40% on average. It shows that the hydrophilic structure can greatly improve the pressure drop for the microchannel condenser.
Chuang, Jason, and 莊志升. "Experimental Study of Heat Transfer in Nanofluid-cooled Microchannel Heat Sink." Thesis, 2005. http://ndltd.ncl.edu.tw/handle/25517146589492126235.
Full text國立中興大學
機械工程學系
93
The major goal of this study is to investigate the microchannel heat sink performance using nanofluids for the coolant. Pure water, nanofluids with volume fraction of 0.204%, 0.25%, 0.294% and 0.4%.and Ethylene glycol- nanofluids with volume fraction of 0.208% are employed in this study. Under the fixed heating power, microchannel heat sink performance in terms of thermal resistance and overall Nusselt number are evaluated bead on the measured with temp variations along the heat sink base plate . The coolant flow rate employed in the rage of 10 to 20 ml/min. As comparedwith the pure water-cooled microchannel heat sink, theexperiment results show the nanofluid-cooled heat sink has better performance when the flow rate is low. At high coolant volume flow rate,nanofluid-cooled microchannel heat sink is worse than pure water–cooled one due to serious nanoparticle agglomeration and deposition. Suitable dispersion agent in nanofluid is required in the heat sink application in order to enhance the device performance.
Chou, Chi-Sheng, and 周記生. "Flow boiling Heat Transfer Enhancement in Porous Microchannel Evaporator." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/38925659236684849096.
Full text國立臺灣大學
機械工程學研究所
100
The microchannel evaporator,which possesses the advantage of high heat transfer coefficient,good temperature uniformity,and small requirement for coolant flow rates,is considered as a potential cooling technology.The porous structure with a large number of nucleation site density as well as the reentrant grooves is to enhance the heat transfer performance in the microchannels evaporator. In present study,the flow boiling experiments were conducted with a plane and porous microchannels evaporator on one square inch copper substrates. Using water as working fluid,the mass flux from103~207 kg/m^2 s and the saturated pressure of 140kpa. Both microchannels have 62 channels(225μm in width;and 660μm in depth).The effects of powder size,thickness of structure upon heat transfer performance are investigated.The comparsions of heat transfer characteristics,pressure drop, pressure instability,and heat transfer enhanced effects between the plane and the porous microchannels evaporator are made.Finally,the comparisons of heat transfer performance,pressure drop,pressure instability between two different working fluid water and R-134a in microchannels. The experiment results were substituted into the heat transfer correlations in which the surface tension force was taken into consideration.The mean average error was16.5%. Pressure drop raised by increasing heat fluxes,but did not vary with increasing mass flux.The experiment results were substituted into the separation model incorporating surface tension force. The mean average error was 21.3%. The pressure drop oscillation suggested that the presence of instability inside plane microchannels as well as the maximum amplitude of oscillation were found near the onset of nucleation. The porous microchannel evaporators were sintered under the following parameters: the powder diameter dp ranged from 1~100μm, thickness of porous structure δ ranged from 225~375μm, and δ/dp ranged from 3~20, respectively. The investigation on the effect of particle size dp as well as thickness δ indicated that the ratio of the thickness to the particle size δ/dp had a significance in the heat transfer performance. This ratio must be properly chosen in order to reach a better heat transfer performance. The better ratio of δ/dp was between 3~4 in our work,withδ 225μm and dp 53μm.The average heat transfer coefficient enhanced about 3 times larger than the plane microchannels. For the porous microchannels evaporator,the heat transfer results different from the plane microchannels evaporator,heat transfer coefficient varied with varing mass flux.Pressure drop in porous microchannel evaporator was raised by increasing heat fluxes.The pressure drop was higher than plane microchannels;however,the maximum pressure drop was not over 50%. The maximum amplitude of oscillation was 66% lower than plane microchannels.This result presented that the porous microchannels evaporator provided a stable boiling behavior when nucleation began. For the porous microchannels: Working fluid water,the better ratio ofδ/dp was between 3~4;however, the better ratio ofδ/dp was between 8~12 when R-134a as working fluid.Surface tension force was probably the different choose between the better ratio ofδ/dp .The comparisons between two different working fluid water and R-134a in microchannels: The pressure results showed that water in the plane microchannels,its maximum amplitude of oscillation was larger than R-134a.The maximum amplitude of oscillation was obviously lower than the plane microchannels in two different working fluids. To conclude the present study, the porous microchannel evaporator is highly potential for the industrial applications
Hsiao, Pang Chi, and 蕭邦佶. "Analysis of Gaseous Flow and Heat Transfer in Microchannel." Thesis, 2001. http://ndltd.ncl.edu.tw/handle/16210586071884750049.
Full text國立中興大學
機械工程學系
89
The major purpose of present study is to investigate the characteristics of flow and heat transfer in a microchannel. The fluid drived by difference pressure at inlet and outlet in laminar flow to investigate compressibility and rarefaction to case the effect of gas flow and heat transfer. In flow, the fluid is assumed to be fully-developed and constant temperature. The investigation shows that the pressure distribution and velocity distribution are the same as Arkilic et al.(1997). Furthermore, the present study employs conservation of mass viewpoint, get the relationship between mass flow rate, inlet/outlet pressure ratio, and the length of microchannel. In heat transfer, the fluid is assumed to be incompressible, the present study is Graetz problem extended to the effect of rarefaction at constant heat flux and constant wall temperature. The investigation shows that the length of thermal fully-developed is longer than traditional heat transfer expected, and Nusselt numbers are decrease with increasing Knudsen number. Furthermore, the study gains Nusselt numbers are function of length of microchannel, and higer Nusselt numbers distribution at higer inlet/outlet pressure ratio when consider effects of compressibility and rarefaction.
Lo, Chung-Yeu, and 羅仲禹. "DSMC of Gaseous Flow and Heat Transfer in Microchannel." Thesis, 2001. http://ndltd.ncl.edu.tw/handle/86644974844481757793.
Full text國防大學中正理工學院
兵器系統工程研究所
89
The study of micro-channel flow is partly in response to the need for thermal control in the operation of MEMS in which the range of gas flow is from slip flow to transition regime. It will lead to incorrect results if we consider gas flow in micro-channel as continuum phenomena. In this paper, molecular approach DSMC has been used to study the flow and heat transfer characteristic of rarefied gas in micro-channel. In one-dimensional simulation, a constant acceleration body force is applied to the system and the flow is restricted in laminar and subsonic state. The simulation results show that the discrepancies of hydrodynamic prediction are widening as indicated from velocity and temperature profiles when the flow in continuum regime transfers to slip flow regime, then low transition regime by increasing Knudsen number(Kn). The data predicted by VHS model differ quantitatively from HS model, but it exists qualitative consistency between them. The macroscopic flow phenomena could be related to and described by the microscopic molecular motion based on simulation results. Pressure-driven flows in micro-channel are simulated by varying inlet/exit pressure for a range of slip to transition regime flows. Both ambient and hot wall temperature cases are investigated. The simulation results of the former case show that the temperature in the flow field is lower than that of the channel wall. It is opposite to one-dimensional flow because of the difference of driving force. It is found that pressure distribution along the channel and streamwise velocity distribution in the transverse direction become more linear and flatter respectively with the increase of the Kn. In addition, the slip velocity increases along the streamwise direction. In hot surface case, the heat flux through the channel wall is more pronounced than in the cold surface case. The flow properties such as temperature, density and pressure are strongly dependent on Kn and heat transfer. The effect of heat transfer from hot wall increases the rarefaction of the flow field and the inlet influence at the same boundary condition. Additionally, the pressure ratio in the flow field is higher than that without heat transfer.