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Unsteady Bulk Boiling in a Tall and Slender Water Pool

机译:高大而细长的水池中的不稳定散装沸腾

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Bulk-boiling processes in large pools are often observed to be extremely non-uniform in time and space, eventually leading to local 'geyser'-like eruptions in turn with relatively quiet, non-boiling temporal phases. For the investigation of such phenomena we have built a tall and flat experimental facility (pool) with transparent walls to allow optical observation of the bulk boiling process at atmospheric pressure. It is heated at its bottom so it can be kept at almost constant temperature conditions for several hours. After heat-up of the entire pool to almost saturation temperature the unsteady boiling process begins randomly in time and space with the appearance of discrete eruptions, associated with the growth of a large number of vapor bubbles. Optical image processing is applied to visualize and track individual bubbles, as well as for the determination of their geometrical parameters. The bubble growth due to the decrease in static pressure is initiated well above the heated surface, i.e. in the 'bulk' region of the pool. The mechanism, which initiates an eruption of bubbles, is identified as a growth-shrinking oscillation of initially small bubbles in the region of upwards rising higher-temperature plumes due to thermal instability and fluid turbulence. It is modeled by a new empirical formula for the number-density of micro-bubbles. A CFD model for the bulk-boiling process has been developed and implemented into the CFX-12 code using the two-fluid formulation of the liquid-vapor two-phase flow. The new formula is applied in the numerical model and the experimentally observed growth and shrinking oscillation is simulated in good qualitative agreement.
机译:通常观察到大型水池中的大量沸腾过程在时间和空间上非常不均匀,最终导致了类似“间歇泉”的局部爆发,进而形成了相对安静,非沸腾的时间阶段。为了研究这种现象,我们建立了一个高而平坦的实验设备(水池),该设备具有透明的壁,可以在大气压下光学观察大体积的沸腾过程。它在其底部被加热,因此可以在几乎恒定的温度条件下保持几个小时。在整个水池加热到接近饱和温度后,不稳定的沸腾过程会在时间和空间上随机开始,并出现离散的喷发,这与大量蒸汽气泡的增长有关。光学图像处理应用于可视化和跟踪单个气泡,以及确定其几何参数。由于静压降低而引起的气泡增长在受热表面上方即池的“散装”区域开始时开始。引发气泡萌发的机制被认为是由于热不稳定性和流体湍流,在向上上升的高温羽流区域中,最初的小气泡的生长收缩振荡。它是由新的经验公式为微气泡的数量密度建模的。已经开发了用于大体积沸腾过程的CFD模型,并使用液-气两相流的两流体配方将其实施到CFX-12代码中。在数值模型中应用了新公式,并以良好的定性模拟了实验观察到的生长和收缩振荡。

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