泡沫铜填充曲折槽道散热器内对流换热研究

设计了高孔隙率泡沫金属铜填充的曲折槽道散热器,采用去离子水为工作介质,实验研究了单相对流换热时散热器的压降、散热量、热阻等特性.结果表明,流体流过槽道时压降和流速成二次多项式关系;随着受热表面温度升高,散热量变大,热阻减小并趋于定值.相同雷诺数时,Nu数随着表面温度的升高而增大;综合评价散热器的性能发现,该换热器在相同压降时热阻要低于微槽道散热器和平板多孔介质散热器.     

微针肋槽道内去离子水换热特性

设计了槽肋比为1:2和2:1的矩形大长宽比微针肋散热器,并实验研究了去离子水在其内的流动换热性能。结果表明:当进口温度为40 ℃、微针肋槽道在雷诺数小于650、最高壁面温度低于77 ℃时,单位面积散热量可达21.32 W/cm2。当雷诺数一定时,同一个槽道壁面温度沿着流动方向不断增加、同一个位置壁面温度随着加热功率的增加而增大,局部努谢尔数沿着流动方向先减小后逐渐增加并趋于定值。当针肋流动换热长度较长时,其入口效应可以忽略,槽道平均努谢尔数随着雷诺数的增大而增大,与加热功率无关;为了更好地表达微针肋槽道内的换热特性,考虑了槽肋比、流动雷诺数等影响,拟合了去离子水在微针肋槽道内的对流换热关系式。     

微针肋内潜热型功能热流体换热特性研究

引入潜热型功能热流体替换现有传统工质冷却大功率激光器,实验研究了潜热型功能热流体与传统工质去离子水在高4 mm、宽2 mm、间距1 mm的微针肋内的层流流动换热特性。结果表明:在雷诺数Re为625~1125范围内,潜热型功能热流体均表现出比水更好的冷却性能及更低的壁面温度,且存在最佳的质量分数值;相同工况下,潜热型功能热流体平均努谢尔数Nu大于去离子水,平均努谢尔数Nu随着雷诺数Re的增加而增加。拟合了平均努谢尔数与流体雷诺数、普朗特数、质量分数的经验的关系式,最大偏差为16.9%,可以较好反映潜热型功能热流体的换热特性;潜热型功能热流体沿着流动长度的方向存在一个稳定的局部换热强化区,且强化换热存在最佳的长度。     

流体在微多孔介质内对流换热实验研究

本文对空气流过烧结微多孔介质内部对流换热进行了实验研究,分析了不同颗粒直径下对流换热努谢尔特数随流量的变化.结果表明:当颗粒直径为200～40μm时,实验得到的对流换热努谢尔特数与已有研究结果符合很好;当颗粒直径为20μm和10 μm时,实验结果略小于已有研究结果,说明空气在微多孔介质中的对流换热需要考虑微尺度效应的影响.同时,根据实验结果给出了微多孔介质内对流换热努谢尔特数与雷诺数的经验关联式,并提出了考虑努森数的修正关联式.     

微方肋冷却系统的换热特性

采用去离子水为冷却介质,对自行设计的不同结构微方肋散热器内的换热特性进行实验研究,结果表明:在进口温度为20 ℃、进口流量为57.225 L/h、底面平均温度为73.4 ℃时,散热器散热量可达2.83106 W/cm2,可以满足当前高热流密度散热需求;当散热面温度一定时,散热量随着散热器进口流量的增加而增加,但增速随散热器底面温度的增加变缓;努谢尔特数随雷诺数的增加而成幂次方增加,常规针肋结构和微针肋结构换热关系式不满足微方肋散热器特性。为了更好地表达微方肋散热器内的换热特性,拟合了微方肋散热器内对流换热关系式。     

束腰结构扰流柱通道的传热和阻力特性

本文对涡轮叶片尾缘中具有束腰结构扰流柱的冷却通道的传热和流动阻力特性进行了实验研究,重点研究了雷诺数、扰流柱的束腰比以及不同组合的影响.结果表明:(1)通道平均努塞尔数随着Reynolds的增加而增大,而当Reynolds数较大时,与圆柱通道相比,束腰结构扰流柱通道的换热效果稍低;(2)通道内平均努塞尔数随着束腰比的增大先增大后降低,然后有所变缓,而其压力损失却曲折波动;(3)在三排扰流柱中,第Ⅱ排束腰结构扰流柱对换热效果影响最大,第Ⅰ排影响最小.当第Ⅰ排和第Ⅲ排为束腰结构扰流柱时,其换热减弱,而压力损失系数却增大.     

微槽道中纳米流体沸腾换热特性研究

为研究纳米流体在微槽道中的沸腾换热特性及规律,分别以去离子水和体积浓度为0.2%、0.5%的水基Al2O3纳米流体为工质进行试验,研究质量流速、热流密度、进口过冷度、槽道尺寸等因素对沸腾传热系数的影响及其两相摩擦压降与出口干度的关联分析和沸腾换热关联式对比拟合.试验结果表明:在一定热流密度和质量流速下,传热系数随槽道尺...     

一种板式换热器一侧流量分配的数值分析

本文以双人字形板式换热器的波纹通道为对象,用数值模拟方法研究了冷侧通道内的流量分配特性与传热特性。发现在单边流情况下,流体经导流区分流后,存在流量分配不均现象。改变导流区结构参数后得出：当雷诺数在2400～12500范围内时,导流区左上侧导流槽角度为60?时流量分配较均匀;左上侧导流槽角度为60?,导流区左下侧导流槽间距为15 mm时,流量分配均匀性更好;在上述两种结构基础上,导流区左下侧角度为180?时,流量分配不均情况改善最佳。在流道中加装封条发现3个封条效果最佳。     

推进剂液体获取装置中多孔筛网的阻力特性研究

荷兰斜纹筛网是推进剂液体获取装置(LAD)中气液分离的核心部件,通过分析通道式表面张力液体获取装置内低温流体流过多孔筛网的过程,构建了三种不同目数筛网的数值计算模型。采用改变液体获取装置进出口压差的方式,研究了筛网在不同进口速度、不同低温流体情况下的阻力特性。结果表明,越靠近LAD出口管道处流体速度越大,压降越大,当进口速度u=0.022 m/s时,DTW 200×1 400筛网下方的流体压力较上方减小了23.4%～31.1%;编织密度越高的筛网,流动阻力越大,产生的压降越大;相同进口速度下,液氧的压降最大,液态甲烷次之,液氢最小,当进口速度u0.2 m/s时三种流体的压降数值差异较小,随着进口速度逐渐增大,三种流体的压降差距呈非线性增大;通过阻力系数和孔隙雷诺数的计算结果得出了适用于荷兰斜纹筛网的阻力系数关系式f=8.79/Re_p+0.39。     

含内热源多孔介质–自由流通道内非达西强制对流

基于多孔介质局部非热平衡模型,对考虑内热源条件下的多孔介质–自由流耦合通道内非达西对流换热特性进行研究。多孔介质区内流体运动方程采用Darcy-Brinkman-Forchheimer模型,利用有限差分法获得通道内各区域流体运动速度、流固相温度分布及努塞尔数,并进一步分析了相关参数对流体流动传热的影响。结果表明：在文中研究参数下,惯性参数F_f对通道内各区域流体速度及温度分布的影响仅在达西数Da大于10^-3时需要考虑;增加F_f或降低固相内热源W_s绝对值会使流固两相温差减小,且改变固相内热源换热方向会使多孔介质区内流固相发生温度分岔现象;固相内热源对通道换热效果影响较大且更为复杂,不同惯性参数F_f下,考虑W_s时可能会使Nu出现奇异点。     

Thermo-Hydraulic Behavior of Microchannel Heat Exchanger System

This article presents an experimental study of thermo-hydrodynamic phenomena in a microchannel heat exchanger system. The aim of this investigation is to develop correlations between flow/thermal characteristics in the manifolds and the heat transfer performance of the microchannel. A rectangular microchannel fabricated by a laser-machining technique with channel width and hydraulic diameter of 87 μm and 0.17 mm, respectively, and a trapezoidal-shaped manifold are used in this study. The heat sink is subjected to iso-flux heating condition with liquid convective cooling through the channels. The temporal and spatial evolutions of temperature as well as total pressure drop across the system are monitored using appropriate sensors. Data obtained from this study were used to establish relationships between parameters such as longitudinal wall conduction factor, residence and switching time, and thermal spreading resistance with Reynolds number. Result shows that there exist an optimum Reynolds number and conditions for the microchannel heat exchanger system to result in maximum heat transfer performance. The condition in which the inlet manifold temperature surpasses the exit fluid temperature results in lower junction temperature. It further shows that for a high Reynolds number, the longitudinal wall conduction parameter is greater than unity and that the fluid has sufficient dwelling time to absorb heat from the wall of the manifold, leading to high thermal performance.     

涡轮叶片前缘阵列冲击冷却流动及传热特性数值研究

本文采用SST湍流模型模拟了类前缘通道内蒸汽射流阵列冲击冷却的流动与传热特性,分析了雷诺数(Re =10000～50000)、孔径比(d/H= 0.5?0.9)和孔间距比(S/H = 2～6)对流动及传热性能的影响规律,得到了相应的传热和摩擦关联式.结果表明:在不同雷诺数下,d/H从0.5到0.9变化时,通道压力损失系...     

Experimental Investigation of the Effect of Flow Arrangements on the Performance of a Micro-Channel Heat Sink

Abstract

An experimental study is carried out to investigate the effect of entrance and exit conditions that prevail due to different flow arrangements on the thermal performance of a copper micro-channel heat sink. Three flow arrangements—U-type, S-type, and P-type—were considered for the analysis with a test piece having inlet and outlet plenum dimensions of 10 mm × 30 mm × 2.5 mm with an array of parallel micro-channels having an individual width of 330 μm and a uniform channel depth of 2.5 mm. Performance evaluations for different flow conditions at inlet and outlet plenums were made by maintaining constant heat supply at 125 W, 225 W, and 375 W with varying Reynolds number ranging from 224 to 1,121. Nusselt number and pressure drop were computed by measuring temperature difference and pressure drop across the inlet and outlet plenum for various test combinations. Maximum heat transfer was observed for the U-type flow arrangement, followed by the P-type and S-type; maximum pressure drop was noted for the S-type flow arrangement, followed by the U-type and P-type arrangements for a constant Reynolds number. A detailed analysis of the experimental results indicate that from a pressure drop point of view, the P-type flow arrangement is preferred, whereas from the heat transfer point of view, the U-type is found to be a better option.     

内嵌微流道低温共烧陶瓷基板传热性能（英）

随着系统级封装（SIP）所容纳的电子元器件和集成密度迅速增加,传统的散热方法（热通孔、风冷散热等）越来越难以满足系统级封装的热管理需求。低温共烧陶瓷（LTCC）作为常见的封装基板材料之一,设计并研制了三种内嵌于LTCC基板的微流道,其中包括直排型、蛇型和螺旋型微流道（高度为0.3 mm,宽度分别为0.4, 0.5和0.8 mm）。通过数值仿真和红外热像仪测试相结合的方式分析了微流道网络结构、流体质量流量、雷诺数、材料热导率对内嵌微流道LTCC基板换热性能的影响,实验结果表明:当去离子水的流量为10 mL/min,热源等效功率为2 W/cm2时,直排型微流道的LTCC基板最高温度在3.1 kPa输入泵压差下能降低75.4 ℃,蛇型微流道的LTCC基板最高温度在85.8 kPa输入泵压差下能降低80.2 ℃,螺旋型微流道的LTCC基板最高温度在103.1 kPa输入泵压差下能降低86.7 ℃。在三种微流道中,直排型微流道具有最小的雷诺数,在相同的输入泵压差下有最好的散热性能。窄的直排型微流道（0.4 mm）在相同的流道排布密度和流体流量时比宽的微流道（0.8 mm）能多降低基板温度10 ℃。此外,提高封装材料的热导率有助于提高微流道的换热性能。     

波纹板式空冷器阻力与传热特性实验研究

在可改变风量和热水流量的实验条件下,对波纹板式空冷器的阻力与传热特性进行实验研究。得到了空气侧的阻力降关联式以及两侧的对流换热系数关联式,其适用于热水雷诺数在2000-8000之间、空气雷诺数在2000-10000之间。在相同工况下,比较了波纹板式、光管式和翅片管式空冷器的性能指标,结果表明:迎面风速在2.45-4.1 m/s之间,波纹板式空冷器传热系数达到100-160 W/m2/℃;约比光管式提高70%,但只有以管束外表面为基准的翅片管式传热系数的六分之一;板式空冷器单位体积换热量约是翅片管式空冷器的1.5倍,是光管式的15倍;板式空冷器单位功耗换热量约是光管式空冷器的5.5倍,而翅片管式空冷器与光管式空冷器则相差不大。     

厚翅片管内流体流动和传热的数值分析

本文应用Ｐａｔａｎｋａｒ等人［１］研究薄翅片管的湍流模型，对一种工业化的厚翅片管内的流体流动和传热进行了数值分析。计算范围包括了层流和湍流（Ｒｅ＝１０１～１０６），所得计算结果与较窄范围内实验所测的传热与阻力数据相当符合，本计算结果具有较大的推广价值。     

Numerical study of heat transfer enhancement of counter nanofluids flow in rectangular microchannel heat exchanger

This paper reports a numerical analysis of the performance of a counter-flow rectangular shaped microchannel heat exchanger (MCHE) using nanofluids as the working fluids. Finite volume method was used to solve the three-dimensional steady, laminar developing flow and conjugate heat transfer in aluminum MCHE. The nanofluids used were Ag, Al₂O₃, CuO, SiO₂, and TiO₂ and the performance was compared with water. The thermal, flow fields and performance of the MCHE were analyzed using different nanofluids, different Reynolds numbers and different nanoparticle concentrations. Temperature profile, heat transfer coefficient, pressure profile, and wall shear stress were obtained from the simulations and the performance was discussed in terms of heat transfer rate, pumping power, effectiveness, and performance index. Results indicated enhanced performance with the usage of nanofluids, and slight penalty in pressure drop. The increase in Reynolds number caused an increase in the heat transfer rate and a decrease in the overall bulk temperature of the cold fluid. The increase in nanoparticle concentration also yielded better performance at the expense of increased pressure drop.     

Experimental studies on natural convection of water in a closed-loop vertical annulus

Experimental studies on heat transfer and fluid flow of water in a vertical annulus, circulating through a cold leg forming a closed loop thermo-siphon, have been carried out in this article. The annulus has a radius ratio (outer radius to inner radius) of 1.184 and aspect ratio (length to annular gap) equal to 352. The experiments were conducted for constant heat fluxes of 1, 2.5, 5, 7.5, 10, 12.5, and 15 kW/m². Transient behavior during the heat-up period of the system until the steady-state condition is attained and discussed. Variation in the heat transfer coefficient and Nusselt number along the annulus height represent the developing boundary layer at the entrance and fully developed flow in the remaining length. A large drop in the differential pressure is experienced when the liquid is circulated through the flow meters, which restrict the flow due to their very small passages. Flow restriction causes mass accumulation and rise of pressure at the exit of the annulus. It also causes a decrease in liquid head in the cooling leg. An increase in the heat flux leads to an increase in the heat transfer coefficient and Nusselt number. As a result of the data analysis correlations for the average Nusselt number, Reynolds number and circulation rate have been developed in terms of the heat flux.