共查询到19条相似文献,搜索用时 125 毫秒
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微细板翅与烧结多孔结构中对流换热实验研究 总被引:2,自引:0,他引:2
本文对水和空气流过4个微细板翅结构和1个烧结多孔结构中的对流换热进行了实验研究,并对其流动与对流换热性能进行了分析和比较。结果表明:在本文实验参数范围内,与空槽道相比,这4种微细板翅结构分别使水的对流换热系数增加10—24倍,分别使空气的对流换热增强了16~40倍;与相同孔隙率的烧结多孔结构相比,微细板翅结构中的流动阻力相近,而对流换热系数却增大。存在最优的微细板翅结构,其换热性能大大强于烧结多孔结构,而流动阻力更小。 相似文献
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研究非共沸混合工质R32/R134a(质量比,25%/75%)在水平微尺度通道内流动沸腾换热规律。在各种工况下进行了非共沸混合工质R32/R134a在水平微尺度管道内流动沸腾换热的实验,考察了质量流量G、热流密度q、质量干度x对微尺度通道内流动沸腾换热系数的影响。研究表明:在热流密度、质量流量都较低的区域,对细管道,换热系数与热流密度的关联度较大;而对微管道,换热系数受影响的因素比较多,并在干度为0.6时出现"干涸"现象,使得换热系数急剧下降。在质量流量高的区域,对细管道,热流密度对换热系数的影响很小;而对微尺度管道,当干度为0.06时换热系数发生转变,随质量干度的增加先减小后增大,热流密度增大到一定的阶段后,换热系数不再随热流密度变化。 相似文献
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本文采用拍摄速度为10000帧/秒的高速摄影仪对不锈钢箔表面的过冷沸腾现象进行了可视化实验研究。实验结果与用微液层模型理论预测的结果一致。高过冷度区域的沸腾换热机理主要是由气泡生长、消失过程中温度边界层的强制排除(所谓强制对流)引起的。气泡周期主要由等待时间构成,这在过冷度高的情况下尤为显著。对等热流密度换热面,微液层模型预测的气泡周期与实验值比较吻合。 相似文献
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Microfin arrays with fin heights of 100 and 200 μm are fabricated, and natural convection around microfin arrays on a vertical surface is experimentally investigated. Microfins are fabricated by DRIE in a bulk silicon wafer. The array spacing investigated ranges from 30–360 μm, and the temperature difference between the wall temperature of the microfin array and the ambient temperature varies from 20–80 K. For comparison, minifin arrays with a fin height of 1 mm are also tested. The heat loss through the backside of the arrays was avoided by a symmetric design of fin arrays on the vertical surface. The convective heat transfer coefficients are measured and compared with the existing heat transfer correlation for the microfin arrays. It turns out that the heat transfer correlation for macrofin arrays is inadequate for the accurate estimation of the heat transfer rate in microscale systems. In addition, microfin and minifin arrays are also tested on a horizontal surface to examine the orientation effect at small scales. 相似文献
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M.R.G. Zoby S. Navarro-Martinez A. Kronenburg A.J. Marquis 《Proceedings of the Combustion Institute》2011,33(2):2117-2125
Studies of regularly ordered droplet arrays facilitate the analysis of local effects on evaporation rates. This work investigates, using Direct Numerical Simulations (DNS), the effects of droplet density and flow conditions on evaporation of kerosene droplets in inert and reactive convective environments. A novel model, coupling a mass conservative Level Set approach with the Ghost Fluid method, is used. The rates obtained from the DNS are compared to two evaporation models based on heat and mass transfer numbers commonly used for RANS methods and Large Eddy Simulations (LES). The results show that predictions of evaporation rates of dense sprays using these models has a limited success. The use of the 1/3-rule to calculate mixture properties results in underpredictions of the evaporation rates by around 20% to 50% in most of the cases studied. The models can only predict the DNS results accurately with errors lower than 2%, if the properties in the evaporation rate models are based on properties in the near field around the droplet. Further studies on the effects of turbulence on the evaporation process showed no evident correlation between the evaporation rates and the subgrid kinetic energy relating the effects of turbulence to vapour dispersion away from the droplet surface. 相似文献