共查询到18条相似文献,搜索用时 88 毫秒
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采用计算流体力学(CFD)方法,对小型脉冲管制冷机进行了二维数值模拟,研究了脉冲管制冷机部件变截面处的结构非对称性对流场的影响。数值模拟结果观测到由非对称结构所引起的非对称流动,揭示了第三直流效应的产生机理,这种非对称流动以周期性演变的涡量环流的形式进行。涡量环流的演变是一个能量的耗散过程,文中还对比了不同输入功率和运行频率对涡量耗散的影响。此外,将数值模拟结果与实验实测结果进行对比,验证了数值模拟的有效性,并从涡量耗散的观点出发对小型脉冲管制冷机输入功率增加到一定程度后制冷温度升高的反常现象进行了解释。 相似文献
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细小圆管内液体流动特性实验研究 总被引:2,自引:0,他引:2
本文实验研究了去离子水在直径为 1.0~2.0 mm 的细小圆管中的流动阻力特性.通过比较相同直径、不同管长的压差,获得了摩擦因子及局部损失系数随 Re 数变化关系.本文实验条件下,对于不同直径的细小圆管,沿程压降及局部压降随流速变化趋势一致;随着管径减小,摩擦因子也减小,且在层流区和湍流区内均要比常规尺度条件下的小;对于不同直径的细小圆管,局部损失系数随 Re 数变化趋势基本一致,当 Re 数相同时,管径越小,对应的局部损失系数越大;对于直径为 1.0~2.0 mm 的细小圆管,临界雷诺数 Rec=2050~2300. 相似文献
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变截面微石英管内流动特性分析 总被引:2,自引:0,他引:2
以去离子水作为工质,流经内径分别为304.13 μm和192.87 μm的石英管所连接而成的变径微管道,根据压降与流量的变化关系,研究微管道内过流截面突然扩大和缩小时微管内阻力特性.利用常规管路阻力损失计算方法对管路的阻力进行计算,并与实验值相比较.研究表明,当雷诺数Re(大直径微管)低于500时,微尺度变截面管路流阻的实验值近似等于常规管路阻力计算公式的计算值;当Re数大于500时,实验值与理论值产生偏差,并且随着雷诺数的进一步增大两者偏差越来越大. 相似文献
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本文将一种VLES(Very Large Eddy Simulation)模型引入到动网格数值计算中,并验证了VLES模型用于模拟类似振动圆柱绕流的动边界问题的有效性.数值求解了不同振幅和频率下非稳态振动圆柱绕流问题.研究表明:随着振幅和激励频率的增加,绕圆柱流动涡脱离形式从2S模式转换到2P0模式,再到P+S模式.在... 相似文献
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This article presents the experimental results of an evaluation of the influence of internal flow patterns on the heat transfer performance of a closed-loop oscillating heat pipe with check valves. It was found that the internal flow patterns could be classified according to four flow patterns: dispersed bubble flow, bubble flow, slug flow, and annular flow, respectively. The main regime of each flow pattern can be determined from a flow pattern map. The map can be used to predict the trend of the heat transfer rate in the closed-loop oscillating heat pipe with check valves. 相似文献
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研究了钛宝石激光器增益介质两端的两块双色镜的相移色散,发现反射相移在中心波长附近发生了突变,由此而造成反射相移色散在此点是不连续的,并对影响反射相移突变点的因素进行了详细的研究。 相似文献
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对流动分岔后的超临界二氧化碳在平面对称突扩管中进行强迫对流换热进行了数值模拟,研究了热流密度在流体发生流动分岔现象后流动特性的影响。计算结果表明:随着热流密度的增加,临界雷诺数和转换雷诺数减小,流动稳定性遭到削弱;对应于相同的雷诺数,由于流动分岔引起的不对称压力分布随着热流密度的增加对应于突扩管上、下半部有不同变化规律,这使得对应回流区的大小分别减小和增大。 相似文献
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The flow characteristics of the trailing edge of vertical vanes installed at the intersection of a T-junction duct were experimentally investigated using particle image velocimetry. The measured velocity field in the branch duct with/without single circular cylinder was studied under different cross velocities and velocity ratios. Additionally, the effect of the locations of cylinder on the flow field was discussed. The positive velocity region, the unsteady flow region and the trailing edge flow region of the vane, have been observed. The positive velocity region existed in almost one half of the measured area. As for the unsteady flow region, the unstable double-vortex structure transformed into a single-vortex structure as the velocity ratio increased. As for the trailing edge flow region of the vanes, the vortex streets could be visualised. Furthermore, the location of cylinder has revealed significant influence on the flow distributions in the trailing edge flow regions of the vanes. The flow structure without cylinder in the measured area is dependent on combinations of the cross velocity and velocity ratio, whereas that with cylinder is dependent on the velocity ratio. The vorticity fields were analysed in each region, and the velocity components revealed the cause of airflow trajectory. 相似文献
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Abstract Flow through a blade trailing edge passage has been experimentally investigated in this article. This rectangular passage is divided into two channels by either a straight or a 120° wavy partition. Fluid in the first channel was injected into the second channel via 14 openings (holes) distributed uniformly and in the crests and troughs for the wavy configuration. Particle image velocimetry and a charge coupled device camera were used in experiment, with Reynolds number varying from 1,800 to 6,700. Experimental results show that the wavy configuration produces an oscillation flow in the second channel. The cause for the oscillation may due to the 120° wavy partition causing shear-layer instabilities and the formation of spanwise eddies by the wavy board. Pictures from the charge coupled device camera revealed strong mixing in the trailing edge, and this mixing could enhance heat transfer, which was confirmed in previous research. The amplitude of oscillation depends on Reynolds number and hole positions. It was observed that the injection flow was not symmetric to the openings, and it was skewed to the direction of the first channel main flow. The ratio of flow rate through the outlet and the bleeding holes was from 1:1 to 1:3. 相似文献