共查询到19条相似文献,搜索用时 140 毫秒
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本文面向电蓄热采暖应用设计了一种新型内嵌式热管,通过可视化和传热实验研究了充液率在5%至70%之间变化时热管内部的流型演化规律和传热特性。根据流型演化过程可以将充液率分为小、中、大三个类别。小充液率时,热管内部出现间歇剧烈沸腾过程;中等充液率时,热管内部出现持续沸腾现象,冷凝段受到搅混流的周期性冲刷;大充液率时,气液混合工质在绝热段往复振荡,冷凝段始终存在液态工质。对于充液高度小于加热段高度和充液高度大于加热段高度两种情况,随着充液率的增大,热阻均先降低后升高,但充液高度大于加热段高度时的热阻普遍大于充液高度小于加热段高度时的热阻。10%充液率时热阻最小,80 W加热功率时约为0.017℃/W,此时蒸发段为持续薄液膜蒸发传热,冷凝段为周期性扰动冷凝和强制对流耦合传热。 相似文献
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为了研究液氢温区脉动热管在冷却Mg B2超导磁体方面的可行性,利用浙江大学制冷与低温研究所现有的实验平台,进一步开展了液氢温区脉动热管的实验研究。在低弯头数(N=2)下,充液率55.8%的脉动热管在加热功率0.1W时可以启动;随着加热功率增大,经历了启动、脉动、极限三个阶段,启动阶段脉动热管传热温差波动很大、传热性能差,而脉动阶段脉动热管传热温差很小、传热性能好。在加热功率0.6W、充液率27.8%时,脉动热管具有最大的传热系数68k W/(m·K),此时蒸发段和冷凝段的温差为0.29K。 相似文献
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分离式热管换热器传热特性的实验研究 总被引:1,自引:0,他引:1
本文在自行设计分离式热管实验装置的基础上,对其传热特性进行了实验研究。其工作温度为170~250℃,热流密度为25~50 kW/m~2。蒸发段和冷凝段构成相同,均是由7根直径30 mm的无缝钢管短管束组成,管长为160 mm,带有紧套的钢帛环形肋片结构尺寸为:外径45 mm、厚1 mm、片间距4 mm。实验结果表明,在本实验条件下,分离式热管的最佳充液率按管束总容量计为18%~38%。根据实验结果拟合了最佳充液率(24%)下蒸发段内部平均沸腾换热系数和冷凝段内部凝结换热努塞尔数综合关系式。 相似文献
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以R600A为工质的分离式热管的实验研究 总被引:1,自引:0,他引:1
对分离式热管的整体热量传递特性进行了实验研究。以蛇形翅片管作为冷凝段和蒸发段进行热管实验,探讨了蒸发器进风面风温及分离式热管蒸发器与冷凝器之间高度差、工质充注量对分离式热管的影响。实验表明,随着蒸发器进风温度的升高,蒸发器与冷凝器换热系数都是呈现先增大后减小的趋势。在冷凝端进风温度恒定为16.55℃、蒸发端进风温度低于60℃时,以R600A为工质的分离式热管的传热量曲线近似于二次曲线,蒸发端进风温度高于60℃时,其传热量曲线近似于一条直线。加大充液率及增加蒸发器与冷凝器的高度差,分离式热管的传热能力均会得到提高。 相似文献
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The aim of this research was to investigate the flow patterns and heat transfer of a top heat mode closed-loop oscillating heat pipe with check valves (THMCLOHP/CV). In this study, the heat pipe was made of a high-quality glass capillary tube with an inner diameter of 2.4 mm bent into 10 meandering turns. The number of check valves was 2 and the tube was filled with R141b at a filling ratio of 50% of internal volume of the tube. The combined lengths of the evaporator, adiabatic and condenser sections were equal to 50 mm. The pipe was operated at the top heat mode, and the angles of inclination were 20°, 40°, 60°, 80°, and 90°. The heat applied at the evaporator section was controlled at 85°Cto 105°C, and 125°C. The results show that in the evaporator section, bubbles are produced and grow as a result of the continuous nucleate boiling. They coalesced and their volume expanded. Similarly, in the condenser section the vapor plug condensate caused the bubbles to collapse and accumulate as a liquid mass at the lower section of the U-bend tube. A new slug then developed and the bubbles coalesced in an upward flow. Heat flux increased when the evaporator temperature and inclination angle increased causing the average length of the vapor plug to decrease and the average velocity of vapor plug to increase. The maximum heat flux occurred at an evaporator temperature of 125°C and an inclination angle of minus 90°. 相似文献
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实验研究燕尾形轴向槽道热管启动/关闭及负荷变化的瞬态响应特性。建立了燕尾形轴向槽道热管的热阻理论预测模型,分析工作温度和热负荷及对热管总热阻的影响。结果表明:热管在负荷突然增加或减小时,响应特性良好;热管在启动过程中,热管的蒸发段、绝热段和冷凝段的温度都在增大;总热阻随热负荷的增大而增大;然而,总热阻受工作温度的影响较小;比较总热阻和平均温差的实验测量和计算值,两者符合较好。 相似文献
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《Heat Recovery Systems and CHP》1991,11(4):313-319
An equation to determine the optimum position of the partition separating a heat pipe into evaporator and condenser regions in a heat pipe heat exchanger was formulated by minimizing the total thermal resistance of the heat path. The optimal position of the partition plate for various operating conditions was found and analysed. Some improvements of thermal efficiency could be achieved. 相似文献
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The sorption heat pipe (SHP) is a new heat transfer device, which can be used as a sorption cooler or as a heat pipe. The SHP has a sorbent bed (adsorber/desorber and evaporator) at one end and a condenser+evaporator at the other end. This device is insensitive to some “g” acceleration and could be suggested for space and ground application. The most crucial feature of this device is that in different cases it can be used, for example, as a loop heat pipe, because they have the same evaporator and condenser, or as a SHP. The SHP can be used also as a cryogenic cooler. The SHP is convenient for cryogenic fluid storage, when the system does not work at low pressure and room temperature, and for use in the active cryogenic thermal control systems of spacecraft in orbit (cold plates for infrared observation of the Earth or space), or as an efficient electronic component cooling device. 相似文献
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《Heat Recovery Systems and CHP》1994,14(4):351-363
A transient lumped heat pipe formulation for conventional heat pipes is presented and the lumped analytical solutions for different boundary conditions at the evaporator and condenser are given. For high temperature heat pipes with a radiative boundary condition at the condenser, a nonlinear ordinary differential equation is solved. In an attempt to reduce computer demands, a transient lumped conductive model has been developed for noncondensible gas-loaded heat pipes. The lumped flat-front transient model was extended by accounting for axial heat conduction across the sharp vapor-gas interface. The analytical solutions for conventional and gas-loaded heat pipes were compared with the corresponding numerical results of the full two-dimensional conservation equations and experimental data, with good agreement. 相似文献
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《Heat Recovery Systems and CHP》1995,15(7):665-673
This paper presents an investigation of the feasibility of heat recovery from the condenser of a vapour compression refrigeration (VCR) system through a Canopus heat exchanger (CHE) between the compressor and condenser components. The presence of the CHE makes it possible to recover the superheat of the discharged vapour and utilize it for increasing the temperature of the external fluid (water) removing heat from the condenser. The effects of the operating temperatures in the condenser and evaporator for different inlet water temperatures and mass flow rates on the heat recovery output and its distribution over the condenser and CHE (the fraction of the condenser heat available through the CHE), available outlet water temperature and heat recovery factor have all been studied and optimum operating parameters for feasible heat recovery have been ascertained. The parametric results obtained for different working fluids, such as R-22, R-12, R-717 and R-500, have been presented. It is found that, in general, a heat recovery factor of the order of 2.0 and 40% of condenser heat can be recovered through the Canopus heat exchanger for a typical set of operating conditions. 相似文献