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径向热管传热的数值计算及结果分析 总被引:1,自引:0,他引:1
采用计算流体力学软件首先对无吸液芯径向热管管壁的温度进行数值计算,其次模拟无吸液芯径向热管中蒸汽的层流对流换热的情况,得出其温度场分布和速度场分布,并对结果进行分析。 相似文献
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《工程热物理学报》2018,(12)
开展了矩形槽道铝-乙醇小型重力热管的传热特性的实验研究,分析讨论了充液率对壁面温度分布、气液两相分布、热阻等热管传热性能的影响。研究表明,充液率对高热负荷工况的两相流动状态和传热特性有显著影响。两相脉动是高热负荷工况小型重力热管特有的两相流动现象.低充液率时,液塞易被气流冲破形成环状流,壁面温度几乎无波动。中等充液率时,在蒸汽和液塞的交替冲刷作用下,热管各段壁面温度均表现出脉动特性。高充液率时,液塞脉动速度的减小削弱了液塞对壁面的冲刷作用,壁面温度未出现明显波动.并且,中等充液率工况下气液两相的快速脉动增强了热管的传热性能,使得均温性和传热极限均优于低充液率和高充液率的情况. 相似文献
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流动沸腾系统中,压降振荡是系统不稳定性的主要型式之一。过载条件下流动沸腾压降振荡缺乏研究。本文采用数值仿真方法,对过载条件下管内流动沸腾的压降振荡特性进行了研究。建立了不同重力条件下压降振荡计算的数学模型,基于此,对过载条件下R134a在2.168 mm水平管内的压降振荡进行了仿真分析,得出了1.41 g、3.16 g(g=9.8 m/s^2)过载条件下的压降振荡特性及其引起的流量振荡、流体温度振荡和壁温振荡,并与对常重力(1 g)下的压降振荡特性进行了对比。结果表明,随着重力增加,流动特性N曲线的负斜率段缩短;一定条件下,当过载增加时,系统从稳定状态趋于不稳定状态。 相似文献
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本文描述了一种新型的太阳能热管喷射式制冷系统。其中热管吸液芯分别采用普通不锈钢丝和反向槽道毛细结构,分析其工作性能。另外为了获得更好的系统COP值,选择四种适合热管工作的工质进行计算,分析它们在采用前述两种吸液芯时的工作情况。研究表明由于反向槽道毛细结构可使工质流动压降更低,增强传热,当系统发生温度为70℃左右时,该系统具有更好的运行性能。而且此系统可有效利用太阳能,该系统若能与建筑复合,则具有广阔的应用前景。 相似文献
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流速对混合蒸汽Marangoni凝结换热影响的实验研究 总被引:1,自引:0,他引:1
本文在蒸汽压力为47.36 kPa的条件下,通过实验研究了不同蒸汽流速(u=2、4、5 m/s)下纯水和不同酒精浓度水-酒精混合蒸汽沿重力方向流过竖直紫铜平板表面上的凝结换热特性,并实现了实验的可视化,同时分析了不同蒸汽流速下造成Marangoni凝结换热特性差异的原因.实验及分析结果表明,在相同蒸汽浓度、蒸汽压力和表面过冷度条件下,高流速下的凝结换热系数比低流速的大.且蒸汽流速对凝结换热的影响因混合蒸汽酒精浓度的不同而不同,低浓度0.5%和高浓度50%时流速的增加对凝结换热特性的影响较小,而在中间浓度2%时凝结换热强度随流速的增加明显. 相似文献
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对制冷剂二氟乙烷(HFC-152a)在内径为8mm的水平管内进行了两相流动沸腾摩擦压降的实验测量.实验测量的压力范围为0.19—0.41MPa,热流密度范围为14—62kW/m2,流量范围为128—200kg/m2s.实验测量表明:HFC-152a的两相摩擦压降随质量流量、质量含气率的增大而增大;热流密度则对摩擦压降的直接影响很小,但通过影响两相流流型间接影响了摩擦压降;当流型由分层流动转变为半环状流或环状流时,总压降中加速压降所占比例有所减小,而摩擦压降所占比例则有所增大;摩擦压降随饱和压力的增大而减小.使用两个应用广泛的压降计算式进行了计算.实验测试结果与计算结果对比后发现,Friedel模型与实验结果偏差较大,而Müller-Steinhagen-Heck模型则与实验结果符合较好. 相似文献
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蒸气凝结相关问题探讨 总被引:3,自引:1,他引:2
讨论了几个与蒸气凝结相关的问题,指出壁面上球冠形液滴的内外压差和临界半径同样遵循经典的Laplace公式和Kalvin公式;蒸气在冷壁上的冷凝形态主要由后退接触角决定;空气中的水蒸气在换热器表面呈膜状冷凝时换热器的性能优于呈滴状冷凝时换热器的性能。 相似文献
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This article experimentally investigates the thermal performance of the vapor chamber module applied to the high-power light-emitting diodes in natural convection. The flat-plate-type vapor chamber and the lamp-type vapor chamber are provided to solve the heat dissipation problem of the high-power light-emitting diodes. The results show that the spreading resistance and the corresponding temperature difference of the flat-plate-type vapor chamber at 30 W are lower than those of the copper plate by 34% and 4°C, respectively, and are lower than those of the aluminum plate by 56% and 6°C, respectively. Compared with the copper and aluminum plates, the lamp-type vapor chamber at 15 W is reduced about 8% and 12% for the total thermal resistance, respectively. In addition, it is also about 3°C and 5°C lower for the central wall temperature of the lighting side, respectively. This study provides a new thermal management method to solve the heat dissipation of the high-power light-emitting diodes. Furthermore, the vapor chamber can effectively lower the spreading resistance and diminish the hotspot effect. 相似文献
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Heat transfer with vapor condensation inside a longitudinally finned tube is numerically studied. The proposed model considers vapor condensation on two initial flow areas, namely, annular and rivulet. The model allows prediction of pressure difference along the tube length, vapor velocity profiles in the central channel and an interfin groove, and also a velocity profile in the condensate rivulet at the bottom of the interfin channel, local heat transfer coefficients at different fin points, and average heat transfer coefficients over tube section and length. The calculations showed that in the case of vapor condensation in longitudinally finned tubes of a small diameter it is of fundamental importance to divide the flow tube section into a central channel and interfin channels. The governing vapor velocities in these channels may differ by more than an order of magnitude. The reduced vapor velocity, used in engineering calculations, does not reflect the character of dynamic vapor impact on a condensate film on the most part of the heat transfer surface. For tubes with relatively large fins the proposed model describes vapor condensation almost completely,meanwhile, the mass vapor quality by the time of filling of the grooves reaches 0.01–0.05. The highest heat transfer intensification was obtained for “sharp fins” with a high value of the fin head curvature. Comparison of results of calculation by the model with results of the known experiments on water vapor condensation yields a good qualitative and quantitative agreement for low vapor velocities at the channel inlet (under 30 m/s). The wall thermal conductivity coefficient value affects significantly the condensation efficiency. 相似文献