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首页> 外文期刊>International Journal of Heat and Mass Transfer >Solutal natural convection flows in ternary mixtures
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Solutal natural convection flows in ternary mixtures

机译:三元混合物中的固有自然对流

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It is known that the cross diffusion terms generate four different types of solutions to the one-dimensional unsteady diffusion equations for ternary mixtures. The stability of the fluid column corresponding to these solutions can be classified depending on the sign of the first derivative of density with respect to the direction of the gravity vector (i.e. partial derivp/partial derivy) and the sign of (partial deriv~2p/partial derivy~2)/y, where y = 0 is located at the center of the diffusion layer. The type of solution depends on the initial conditions and on the set of diffusion coefficients considered. One type of solution corresponds to a stable fluid column with (partial derivp/partial derivy < 0) and (partial deriv~2p/partial derivy~2)/y > 0. Two types of solutions generate fluid layers with unstable density stratification (partial derivp/partial derivy > 0) and the fourth type shows a fluid layer with (partial deriv~2p/partial derivy~2)/y < 0. We analyzed the unsteady diffusion processes in a ternary mixture under the conditions of experiments carried out to determine the four diffusion coefficients of the ternary system 1,2,3,4-tetrahydronaphthaline-isobutylbenzene-dode-cane (THN-IBB-nC12). These measurements; performed in diffusion cells with an initially stable stratification within the cell, with the denser mixture at the bottom and the lighter at the top; are usually based on the validity of the one-dimensional unsteady diffusion mass transfer equations. The linear stability analysis for the onset of convection in the unstable layers with unstable density stratification (partial derivp/partial derivy > 0) indicates that the critical thickness of these layers depends on the Rayleigh numbers, on the diffusion coefficients and on the initial conditions. To illustrate the flow structures that can be generated in these unstable conditions, we performed numerical simulations for selected sets of diffusion coefficients at different Rayleigh numbers. The results of these simulations are in general agreement with the predictions of the linear stability analysis and indicate that, under specific conditions, the convective motions developed in the cell produce significant departures of the concentration distributions from the pure diffusion situation.
机译:众所周知,交叉扩散项为三元混合物的一维非定常扩散方程生成四种不同类型的解。可以根据密度相对于重力矢量的方向的一阶导数的符号(即偏导数/偏导数)和符号(偏导数〜2p //)来对与这些解相对应的流体柱的稳定性进行分类。偏导数〜2)/ y,其中y = 0位于扩散层的中心。解决方案的类型取决于初始条件和所考虑的一组扩散系数。一种类型的解决方案对应于具有(偏导数/偏导数<0)和(偏导数〜2p /偏导数〜2)/ y> 0的稳定流体柱。两种类型的溶液生成的流体层具有不稳定的密度分层(部分导数/偏导数> 0),而第四种类型显示的流体层具有(偏导数〜2p /偏导数〜2)/ y <0.我们在进行以下实验的条件下分析了三元混合物中的非稳态扩散过程确定三元体系1,2,3,4-四氢萘-异丁基苯-甘蔗(THN-IBB-nC12)的四个扩散系数。这些测量;在扩散池中进行,最初在池中分层稳定,混合物中较浓的混合物在底部,较浅的混合物在顶部;通常基于一维非定常扩散传质方程的有效性。对具有不稳定密度分层(偏导数/偏导数> 0)的不稳定层中对流开始的线性稳定性分析表明,这些层的临界厚度取决于瑞利数,扩散系数和初始条件。为了说明在这些不稳定条件下可能产生的流动结构,我们对不同瑞利数下的选定扩散系数集进行了数值模拟。这些模拟的结果与线性稳定性分析的预测大体上一致,并且表明,在特定条件下,电池中产生的对流运动会导致浓度分布与纯扩散情况发生明显偏离。

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