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Analytical and numerical evaluation of two-fluid model solutions for laminar fully developed bubbly two-phase flows

机译:层流完全展开的气泡两相流的两流体模型解的分析和数值评估

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An analysis of the two-fluid model in the case of vertical fully developed laminar bubbly flows is conducted. Firstly the phase distribution in the central region of the pipe (where wall effects vanish) is considered. From the model equations an intrinsic length scale L is deduced such that the scaled system reduces to a single equation without parameters. With the aid of this equation some generic properties of the solutions of the model for pipes with diameter greater than about 20L (the usual case, since L is of the order of the bubble radius) are found. We prove that in all physically meaningful solutions an (almost) exact compensation of the applied pressure gradient with the hydrostatic force rho(eff) g occurs (with rho(eff) the effective density and g the gravity). This compensation implies flat void fraction and velocity profiles in the central region not affected by the wall, even when no turbulence effects are accounted for. We then turn to consider the complete problem with a numerical approach, with the effect of the wall dealt via wall forces. The previous mathematical results are confirmed and the near-wall phase distributions and velocity profiles are found. With the numerical code it is also possible to investigate the regime in which the pressure gradient is greater than the weight of the pure liquid, in which case a region of strictly zero void fraction develops surrounding the axis of the pipe (in upward flow of bubbles). Finally, the same code is used to study the effect of reducing the gravity. As g decreases, so does the relative velocity between the phases, making the lift force increasingly dominant. This produces, in upward bubbly flows, narrower and sharper void fraction peaks that also appear closer to the wall. (C) 2003 Elsevier Ltd. All rights reserved. [References: 15]
机译:在垂直充分展开的层状气泡流的情况下,对两种流体模型进行了分析。首先,要考虑管道中心区域(壁效应消失)中的相位分​​布。从模型方程式中推导出固有长度尺度L,使得经尺度化的系统减少为没有参数的单个方程式。借助于该方程,找到了直径大于约20L的管道的模型解的一些一般性质(通常情况,因为L约为气泡半径)。我们证明,在所有物理上有意义的解决方案中,都会用流体静力rho(eff)g来(几乎)精确补偿施加的压力梯度(rho(eff)时的有效密度和重力g)。这种补偿意味着即使在不考虑湍流影响的情况下,在不受壁影响的中心区域中,平坦的空隙率和速度分布也没有变化。然后,我们将通过数值方法来考虑整个问题,即通过墙力处理墙的效果。确认了先前的数学结果,并找到了近壁相位分布和速度曲线。使用数字代码,还可以研究压力梯度大于纯液体重量的情况,在这种情况下,围绕管轴(在气泡向上流动的情况下)会形成一个严格为零的空隙率区域)。最后,使用相同的代码来研究减轻重力的效果。随着g的减小,相之间的相对速度也随之减小,从而使提升力越来越占主导地位。这在向上的气泡流中产生更窄和更锐利的空隙率峰,这些峰也似乎更靠近壁。 (C)2003 Elsevier Ltd.保留所有权利。 [参考:15]

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