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1.
It follows from an analysis of existing data that the parameters of boiling heat transfer essentially depend on the thermophysical properties and geometrical characteristics (roughness and thickness) of the heat-release wall. However, it has been impossible, so far, to fully and correctly evaluate the effects of roughness and thickness of the heat-release wall. Probably, that is why, presently, no universal criterial relations exist that enable one to describe the huge amount of available experimental data on boiling heat transfer. This article presents an integration of the experimental data on heat transfer in boiling of various liquids on thick tubes having various thermophysical characteristics and roughnesses.  相似文献   

2.
Summary The electroconvective specific-heat transfer coefficient has been measured in various liquids (methanol, kerosene, silicon oil and ethanol) from a single platinum wire (diameter=0.025 mm) mounted along the axis of a copper cylinder (diameter=53 mm). The heat transfer coefficient has been evaluated under the influence of a.c. and d.c. fields. An a.c. field always causes an enhancement in the heat transfer coefficient. A d.c. field causes an inhibition in heat transfer in methanol. A similar trend is noticed in kerosene, but the heat transfer coefficient increases again as the field is increased. An enhancement in the heat transfer coefficient is observed in silicon oil, and a similar trend is noticed in ethanol, but the heat transfer coefficient decreases again as the field is increased. The effect of cylinder orientation on convection is studied. The efficiency of convection has been calculated for various liquids using an empirical relation. The efficiency obtained in a d.c. field is found to be higher than in the a.c. field. A similar trend is also noticed for the electric Nusselt number.  相似文献   

3.
This article presents the nucleate boiling heat transfer characteristics of acetone at one bar on smooth and enhanced circular stainless steel surfaces (SS 316) of 20 mm diameter for heat flux between 1 and 4 W cm? 2, which mimic the operating condition of a typical immersion electronic cooling system. The experimental heat transfer coefficient from the smooth surface is validated against Borishanski correlation [1] within acceptable limits of ± 5%. The steel smooth surface is enhanced by providing 100 equally spaced indents of 0.5 mm diameter and 0.05 mm depth. The experimental results indicate that the enhanced surface shows a good shift in the boiling curve and thus, enhancing the nucleate boiling heat transfer at a lesser wall super heat when compared to the smooth surface by around 35% for tested condition. The effect of subcooling on nucleate boiling in enhanced surface reveal that the heat transfer coefficient degrade by 40 to 55% for a sub cooling of 5 to 10 K. The influence of material is studied by a similar enhanced surface made of brass and compared for the same working condition. The brass enhanced surface showed an improved of around 50% against the steel-enhanced surface. Also, the influence of fluid is studied by comparing acetone and n-pentane, which showed that the latter an enhancement in heat transfer coefficient of 50% over the former.  相似文献   

4.
It is experimentally established that heat transfer and critical heat flux depend much on both the physical properties of the refrigerant and a number of characteristics of the heat-release wall. Below are analyzed experimental data of different authors and an attempt ismade to understand why critical heat flux values in experimental studies deviate significantly from values calculated by the available models of crisis emergence.  相似文献   

5.
The process of development of the third heat transfer crisis for vertical orientation of the heating surface was studied experimentally. Experiments were carried out with acetone under the conditions of saturation for the pressures in the working volume from 20 to 28 kPa. In all experiments, the third heat transfer crisis was preceded by propagation of evaporation front along the heating surface. The threshold values of heat flux densities, above which a stable vapor film is formed on the whole heating surface, are lower for vertical orientation of this heating surface than for the horizontal one. Data on the threshold heat flux densities and overheating before boiling-up were obtained. Above these values, formation of evaporation fronts was observed. The range of operation parameters corresponding to formation of the sites of unstable film boiling on the heating surface after boiling-up was determined.  相似文献   

6.
水平梯度表面能材料表面上的滴状凝结换热系数   总被引:1,自引:0,他引:1  
本文在均质表面的单个球缺形液滴换热模型和液滴通用尺度分布规律的基础上,结合梯度表面能材料表面的液滴分布和凝结换热特性,得到了一维水平梯度表面能材料表面上的滴状凝结换热计算式。在此基础上,研究了壁面过冷度、接触角梯度、工质物性等参数对梯度表面能材料表面滴状凝结换热性能的影响。结果表明:随着过冷度的增加和凝结工质汽化潜热的增大和表面张力的减小和接触角梯度的增大,平均表面凝结换热系数会增大。  相似文献   

7.
马龙信  路昆 《低温与超导》2021,49(1):96-101
基于空气源热泵在低温寒冷地区运行中遇到的结霜问题,对不同风速工况下,结霜过程中设备性能的变化进行分析,以换热量、换热系数为指标对不同翅型换热器的换热特性进行研究。实验结果显示:换热器结霜过程中,换热过程主要分为初始增加段、换热平稳段、缓慢衰减段、后期平稳等四段,结晶体在增加空气湍流度强化换热的同时,也增加了换热热阻使换热效果变差,因此换热效果本质而言是两种换热效果的综合体现;空气阻力随风速的增大、结霜量的增加而增大,而蒸发压力随着风速的增加而升高、随结霜量的增大而减小;百叶窗翅片表面结霜量大于平翅片,因此平翅片翅型当量换热系数更大,翅片结霜量、当量换热系数随风速的增加而增大,风速由1 m/s增至4 m/s时,结霜量、当量换热系数增加约三倍。  相似文献   

8.
 为了考察切向强迫气流对激光辐照下树脂基复合材料热响应的影响,基于边界层换热理论,研究了切向气流与靶面的对流换热系数和热分解气体对表面热交换的覆盖效应,并用有限差分法对激光辐照下树脂基复合材料的1维热响应模型进行数值求解。数值计算表明:高速切向气流的存在会加速靶材表面与外部环境的热交换,从而明显降低激光对靶材的加热效率;边界层换热理论给出的对流换热系数和覆盖因子是合理有效的,适用于数值模拟切向气流对激光辐照下树脂基复合材料热响应的影响;向靶材表面溢出的热分解气体对靶材表面与外部环境的热交换有一定的抑制作用,但影响较小,基本可以忽略不计。  相似文献   

9.
基于降低污垢热阻的复合强化传热研究   总被引:2,自引:0,他引:2  
复合强化传热的换热系数的增加通常要比单独使用其中的任何一种技术高,但过分增长的污垢热阻会轻而易举地将对流换热系数提高的效果加以抵消。将振动看作不仅仅意味着噪声与元件损坏的能量表达方式,就有可能利用流体诱导的传热元件振动扰动水流,提高对流换热系数;同时,用振动变形清除传热表面积垢,降低污垢热阻,从而形成一种复合强化传热的新方法。  相似文献   

10.
本文针对不同压力条件下不同换热表面结构的毛细结构蒸发器气(?)液相变传热特性进行了实验研究。选取微槽道结构和烧结丝网结构的换热表面分别在蒸发压力为0.86×10~5 Pa、0.91×10~5 Pa、0 96×10~5 Pa、1.0×10~5 Pa、1.5×10~5 Pa、2.0×10~5 Pa条件下进行了传热特性研究并对其实验结果进行对比,结果表明,压力对换热系数有重要的影响,当压力范围为0.86×10~5~1.0×10~5 Pa时,在过热度相同的条件下,随着压力的增加,换热系数呈上升趋势;在较大压力的条件下,换热系数随着过热度的增加呈先升后降的趋势。  相似文献   

11.
The nucleate pool boiling heat transfer of ferrofluid on a horizontal plate in the presence of a non-uniform magnetic field has been studied numerically using Eulerian–Eulerian approach. Also, the wall partitioning model was extended to consider the boiling surface modification by the nanoparticles deposition on the heated surface. Adding nanoparticles causes deterioration in the boiling heat transfer coefficient and void fraction. Moreover, applying the magnetic field intensifies these reductions.  相似文献   

12.
岳平*  张强  李耀辉  王润元  王胜  孙旭映 《物理学报》2013,62(9):99202-099202
本文利用锡林郭勒草原2008年春季近地层涡旋相关系统和铁塔的风、 温平均梯度观测资料, 分析了总体输送系数随梯度Richardson数的变化特征, 建立了动量总体输送系数随大气稳定度、近地层风速以及感热总体输送系数随大气稳定度和近地层气温的关系. 中性条件下, 半干旱草原植被下垫面动量总体输送系数与近地层大气动力状态之间存在明显的相互作用, 总体输送系数与近地面层风速之间满足二次曲线拟合关系; 风速较小时, 大气动力特征对地表粗糙度长度的改变不是很明显, 动量总体输送系数随气流增强而增大; 而当风速较大时, 强风速会使植被高度发生改变, 动量总体输送系数随气流增强而减小. 另外, 感热总体输送系数与近地层气温之间也存在二次曲线关系. 动量总体输送系数与近地层风速之间的关系、感热总体输送系数与近地层气温之间关系的建立为总体输送系数参数化提供了重要途径, 同时该方案避免了对动力学粗糙度长度和热力学粗糙度长度的求解. 关键词: 总体输送系数 参数化 湍流通量 相似性函数  相似文献   

13.
FC-72在竖直壁面上及微小三角型通道内的沸腾传热   总被引:1,自引:0,他引:1  
本文对浸在FC-72液池中的竖直壁面及两个微小三角形通道进行了沸腾实验研究,考虑了管道尺寸对沸腾传热特性的影响。两个微小三角形通道的边长分别为1.5和2.5 mm,水力直径分别为0.87和1.44 mm,长度50 mm,采用铜块上开V型沟槽,再覆盖上透明的玻璃片构成。热流密度由贴在铜块背后的膜状加热器提供。实验得到了沸腾曲线和传热系数,并用DV摄影机拍摄到了沸腾状况。实验结果显示,管道尺寸对沸腾传热特性有显著的影响,CHF值随通道尺寸的减小而减小,小通道在低热流密度时传热系数较大。  相似文献   

14.
Pool boiling heat transfer performances of Cu-Al2O3-coated copper surfaces have been studied experimentally for its potential use in heat transfer applications. In the present study, a two-step electrochemical deposition method is examined. This method provides an easy control on surface properties such as porosity and coating thickness. The deposition method is studied carefully and responsible surface morphology parameters are reported. After performing the pool boiling experiments on coated surfaces with DI water, the maximum critical heat flux of 1800 kW/m2 and heat transfer coefficient of 193 kW/m2 K, which are 68% and 260% higher than that of bare surface, respectively.  相似文献   

15.
This paper studies the heat-release oscillation response of premixed flames to oscillations in reactant stream fuel/air ratio. Prior analyses have studied this problem in the linear regime and have shown that heat release dynamics are controlled by the superposition of three processes: flame speed, heat of reaction, and flame surface area oscillations. Each contribution has somewhat different dynamics, leading to complex frequency and mean fuel/air ratio dependencies. The present work extends these analyses to include stretch and non quasi-steady effects on the linear flame dynamics, as well as analysis of nonlinearities in flame response characteristics. Because the flame response is controlled by a superposition of multiple processes, each with a highly nonlinear dependence upon fuel/air ratio, the results are quite rich and the key nonlinearity mechanism varies with mean fuel/air ratio, frequency, and amplitude of excitation. In the quasi-steady framework, two key mechanisms leading to heat-release saturation have been identified. The first of these is the flame-kinematic mechanism, previously studied in the context of premixed flame response to flow oscillations and recently highlighted by Birbaud et al. (Combustion and Flame 154 (2008), 356–367). This mechanism arises due to fluctuations in flame position associated with the oscillations in flame speed. The second mechanism is due to the intrinsically nonlinear dependence of flame speed and mixture heat of reaction upon fuel/air ratio oscillations. This second mechanism is particularly dominant at perturbation amplitudes that cause the instantaneous stoichiometry to oscillate between lean and rich values, thereby causing non-monotonic variation of local flame speed and heat of reaction with equivalence ratio.  相似文献   

16.
水平螺旋管内超临界CO2冷却换热的数值模拟   总被引:1,自引:0,他引:1       下载免费PDF全文
徐肖肖  吴杨杨  刘朝  王开正  叶建 《物理学报》2015,64(5):54401-054401
采用RNG k-ε 湍流模型对超临界CO2流体在内径为4 mm, 长度2000 mm, 节距为10 mm, 曲率为0.1的水平螺旋管内的冷却换热进行了数值模拟.研究了质量流量、热流量以及压力对换热系数的影响, 并和超临界CO2在水平直管内的冷却换热进行了对比.研究结果表明, 超临界CO2在水平螺旋管内流动产生的二次流强于水平直管内的二次流, 前者的换热系数大于后者; 换热系数随质量流量的增加而增大; 在似气体区, 换热系数随着热流量的增加而增大, 而在似液体区, 热流量对换热系数几乎没有影响; 换热系数峰值点随着压力的升高而下降, 并向高温区偏移.  相似文献   

17.
照明用大功率LED回路热管散热器的研究   总被引:1,自引:0,他引:1  
分析了照明用大功率LED封装的散热特性,提出了一种用于大功率LED系统散热的回路热管;研究了热负荷、倾角、加热方式等对热管的起动性、均温性、热阻等的影响。试验结果表明,所设计的热管散热器的热阻在0.19K/W~3.1K/W之间,蒸发器的均温性被控制在1.5℃以内,满足大功率LED封装的均温性要求,在热负荷为100W时,蒸发器的温度被控制在100℃以下,满足大功率LED结点温度的控制要求。  相似文献   

18.
Technical Physics - A technique is developed to determine the freezing time, thermal resistance, heat transfer coefficient, and cooling power of water droplet on the surface of studied materials by...  相似文献   

19.
雾化喷射冷却的机理及模型研究   总被引:2,自引:0,他引:2  
雾化喷射冷却的换热机理十分复杂,目前其研究还很不成熟。本文从喷射雾滴的特性参数出发,以被冷却表面上形成的喷射液膜为对象,考虑了冷却液体向环境的散热,建立质量、能量守恒方程,得到半经验半解析的雾化喷射换热模型。其中,本文提出真换热系数和显换热系数的概念,认为显换热系数受空间散热影响,而真换热系数只与喷雾动量有关。最后设计了雾化喷射局部换热实验,对模型进行检验,结果表明,该模型能够较好地符合实验所得的换热系数及加热面表面温度沿喷射半径的分布趋势。  相似文献   

20.
气冷涡轮叶片传统热分析中热边界条件的影响   总被引:1,自引:0,他引:1  
以MarkII气冷涡轮叶片为研究对象,考察了换热系数分布对叶片外表面温度分布的影响。首先分别以温度和换热系数实验值作为热边界条件验证了固体导热计算方法和CFD程序的有效性,然后分析了6种典型热边界条件下的叶片外表面温度分布,并与实验值进行对比。由分析结果可知:叶片外表面温度与换热系数紧密关联,经验关联式(层流、湍流)条件下预测得到的温度偏差较大,当换热系数由能考虑边界层转捩影响的CFD计算得到时,预测得到的温度与实验值较为接近。  相似文献   

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