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热管技术已在电子设备散热领域得到广泛应用。热管的传热能力虽然很大,但不能无限加大热负荷。文中讨论了热管的主要极限如沸腾极限、毛细极限、粘性极限、声速极限、携带极限等的理论表达式,就一种实验用微槽平板热管进行了理论计算,得出了毛细极限是实验热管主要传热极限的结论。 相似文献
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实验测定了水平和垂直放置状态下,铜-水交叉齿内螺纹重力热管的传热特性,并与普通铜-水重力热管进行了比较,得出了交叉齿内螺纹对重力热管传热性能的影响.水平放置状态下,交叉齿内螺纹重力热管具有较低的蒸发段温度、轴向温差和热阻,相比普通重力热管其传热极限也有极大的提升.垂直放置状态下,在40 W低加热功率时,交叉齿内螺纹重力热管传热性能低于普通重力热管,随着加热功率的增加,其传热性能实现反超。 相似文献
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建立了多孔毛细芯结构的平板热管在冷凝段不发生堵塞的情况下流动和传热的理论模型,分析了热管在毛细限下的最大传热量和热阻的变化.结果表明,丝网目数的增加和工作温度的升高会增大热管的传热能力,热管工质为水时的传热性能优于工质为丙酮和乙醇时的情况. 相似文献
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重力热管内的两相流型对其工作特性有着至关重要的影响.本文借鉴垂直圆管内两相流型转变的实验研究结果和近饱和自由降膜流始发沸腾的观测结论,通过简化分析,给出重力热管蒸发段内由泡状流向弹状流过渡的流型转变判据.在低饱和蒸汽压和高过冷度下,这种流型转变将导致周期性振荡的两相流不稳定性,这就是喷涌不稳定性;因此,流型转变判据也就是喷涌不稳定性调控判据.文中还结合数值计算实例,指出影响流型转变的重要因素. 相似文献
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N─甲基吡咯烷酮两相闭式热虹吸管传热特性的实验研究 总被引:2,自引:0,他引:2
本文报道了用N—甲基吡咯烷酮(C5H9NO3)为工质以光滑管与三维内翅片管为管壳制成的两相闭式逆流热虹吸管的传热特性。实验结果表明在工作温度为220~350℃,热负荷为8.2~17.3kW/m2范围内光滑热虹吸管蒸发段与凝结段换热系数的积分平均值分别约为1700W/m2·℃和1600W/m2·℃。由于三维翅片的强化传热作用,使三维内翅片热虹吸管蒸发段与凝结段换热系数分别比光滑管增大了20%~40%和70%~160%。实验表明N—甲基吡咯烷酮综合传热性能优于萘,可望作为中温热管工质使用。 相似文献
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螺旋管内气-液两相流截面含气率试验研究和理论模型 总被引:1,自引:1,他引:0
1前言关于螺旋管内气-液两相截面含气率的预报是一个重要的课题。即使只考虑平均截面含气率,也有气液两相间的滑移、各相流速和气相沿流通截面的不均匀分布等影响因素。查阅有关文献[1,2],对螺旋管内气-液两相截面含气率的研究还很不够。因此,本文重点从二方面进行了研究。首先借助快速关闭球阀法,得出三根不同螺旋管平均截面含气率的试验测定结果,考查了螺旋升角和螺旋直径对其产生的影响;其次,按不同流型,依据“分相动量模型”和“漂移流率模型”、得出计算螺旋管内主要流型平均截面含气率的经验关系式。本文研究对象:三… 相似文献
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直接空冷凝汽器理论最佳背压的研究 总被引:5,自引:0,他引:5
为了更好地提高直接空冷机组系统运行的经济性,本文以直接空冷系统为研究对象,以空冷系统的热力模型为基础,综合考虑汽轮机功率与空冷风机耗功率,从理论上探索研究运行工况下的最佳背压以及有关主要因素对最佳背压影响的基本规律,从而为直接空冷机组的冷端优化和经济运行提供指导. 相似文献
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A visual study of internal flow patterns inside an inclined, closed, two-phase thermosyphon at normal operating conditions for several Bond numbers has been conducted. This article describes the effects of varying inclination angles and Bond numbers (Bo) onflow patterns, A copper thermosyphon was used. R123 was selected as the working fluid, with a vapor temperature of 30°C and a filling ratio of 50%. Flow phenomena were observed at selected inclination angles of 90° and 30° from the horizontal axis, with aspect ratios of 30 and 5. The selected external diameters were 12.0 and 28.5 mm. Flow phenomena were also recorded with a standard video camera and a still camera, and the corresponding heat transfer rates were also monitored. It was observed that the basic internal flow patterns could be classified according to the aspect ratios and the Bo as follows: At an aspect ratio of 10 and higher, the annular flow at vertical changes to slug flow in inclined positions for all values of Bo. A thin liquid film always exists in the upper part, promoting heat transfer. In this case, the ratio of heat transfer rates at peak position and those of the vertical (Q / Q90) are almost the same for all Bo. At an aspect ratio of less than 10 and a low Bo, bubbly flow at vertical changes to stratified flow at an inclined position, with bubbly flow in the lower part. Vapor slug is sometimes seen. At an aspect ratio of less than 10 and a high Bo, bubbly flow with a coagulation of bubbles at the vertical position changes to stratified flow with bubbly flow in the upper part, without any vapor slugs. Q / Q90 is comparatively higher than at lower Bo. This result may be attributed to two main factors: (1) there was an area undisturbed by bubbles in the lower part; and (2) no upward vapor slug movement was observed. 相似文献
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An experimental study is presented for the heat transfer characteristics of a rectangular, two-phase, double-loop thermosyphon with water-steam as the working fluid. The evaporator was installed in the middle branch and shared by the two condensers. Local temperature measurements of the core fluid and the wall were made, and the overall heat transfer coefficients of the evaporator, the condensers, and the loop system were obtained and correlated in terms of the fluid properties, heat flux conditions, and the liquid charge level V+. Results show that the overall heat transfer coefficients increase with decreasing V+ and increasing heat flux. The heat transfer performance of the entire system can be viewed as a parallel combination of the thermal resistances of the evaporator and two condensers. Results also confirm the previous findings that if the liquid charge level is below the fractional volume of the bottom connecting tubes, an overheat phenomenon will take place. 相似文献
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