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Comparison of Nucleation Site Density for Pool Boiling and Gas Nucleation

机译:池沸腾和气体成核的成核点密度比较

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It has been well established that the rate of heat transfer associated with boiling systems is strongly dependent on the nucleation site density. Over many years attempts have been made to predict nucleation site density in boiling systems using a variety of techniques. With the exception of specially prepared surfaces, these attempts have met with little success. This paper presents an experimental investigation of nucleation site density measured on roughly polished brass and stainless steel surfaces for gas nucleation and pool boiling over a large parameter space. A statistical model used to predict the nucleation site density in saturated pool boiling is also investigated. The fluids used for this study, distilled water and ethanol, are moderately wetting and highly wetting, respectively. Using distilled water it has been observed that the trends of nucleation site density versus the inverse of the critical radius are similar for pool boiling and gas nucleation. The nucleation site density is higher for gas nucleation than for pool boiling. An unexpected result has been observed with ethanol as the heat transfer fluid, which casts doubt on the general assumption that heterogeneous nucleation in boiling systems is exclusively seeded by vapor trapping cavities. Due to flooding, few sites are active on the brass surface and at most two are active on the stainless steel surface during gas nucleation experiments. However, nucleation sites readily form in large concentration on both the brass and stainless steel surfaces during pool boiling. The pool boiling nucleation site densities for ethanol on rough and mirror polished brass surfaces are also compared. It shows that there is not a significant difference between the measured nucleation site densities on the smooth and rough surfaces. These results suggest that, in addition to vapor trapping cavities, another mechanism must exist to seed vapor bubble growth in boiling systems.
机译:众所周知,与沸腾系统有关的传热速率很大程度上取决于成核位点密度。多年来,已经尝试使用多种技术来预测沸腾系统中的成核位点密度。除了特殊准备的表面以外,这些尝试均收效甚微。本文介绍了在大的参数空间上对气体和表面沸腾进行粗抛光的黄铜和不锈钢表面上测量的成核位点密度的实验研究。还研究了用于预测饱和池沸腾中成核位点密度的统计模型。用于这项研究的液体,蒸馏水和乙醇,分别是中等润湿和高度润湿的。使用蒸馏水已经观察到,对于池沸腾和气体成核,成核位置密度与临界半径的倒数的趋势相似。气体成核的成核点密度高于熔池沸腾。使用乙醇作为传热流体时,观察到了出乎意料的结果,这使人们对沸腾系统中的异相形核仅由蒸汽捕集腔产生的一般假设产生了怀疑。由于溢流,在气体成核实验中,黄铜表面上几乎没有活性位,而不锈钢表面上最多有两个活性位。但是,在池沸腾过程中,容易在黄铜和不锈钢表面上大量形成形核部位。还比较了粗糙和镜面抛光黄铜表面上乙醇的熔池沸腾成核位点密度。它表明在光滑表面和粗糙表面上测得的成核位点密度之间没有显着差异。这些结果表明,除了蒸气捕获腔外,还必须存在另一种机制来使沸腾系统中的蒸气气泡增长。

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