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Mass transfer to/from distributed sinks/sources in porous media.

机译:与多孔介质中的分布汇/源之间的质量传递。

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This research addresses a number of fundamental issues concerning convective mass transfer across fluid-fluid interfaces in porous media. Mass transfer to/from distributed sinks/sources is considered for (i) the slow dissolution of liquid filaments of a wetting non-aqueous phase liquid (NAPL) held in the corners of angular pores or throats and (ii) the fate of gas bubbles generated during the flow of a supersaturated aqueous phase in porous media.;1. Effects of the stability of NAPL films on wetting NAPL dissolution. Wettability profoundly affects the distribution of residual NAPL contaminants in natural soils. Under conditions of preferential NAPL wettability, NAPL is retained within small pores and in the form of thick films (liquid filaments) along the corners and crevices of the pore walls. NAPL films in pore corners provide capillary continuity between NAPL-filled pores, dramatically influencing the behaviour of NAPL dissolution to the flowing aqueous phase by convection and diffusion. A pore network model is developed to explore the dissolution behaviour of wetting NAPL in porous media. The effects of initial NAPL distribution and NAPL film stability on dissolution behaviour are studied using the simulator. NAPL phase loses continuity and splits into disconnected clusters of NAPL-filled pores due to rupture of NAPL films. Quasi-state drainage and fingering of the aqueous phase into NAPL-filled pores is treated as an invasion percolation process and a stepwise procedure is adopted for the solution of flow and solute concentration fields. NAPL film stability is shown to critically affect the rate of mass transfer as such that stable NAPL films provide for more rapid dissolution. The network simulator reproduces the essential physics of wetting NAPL dissolution in porous media and explains the concentration-tailing behaviour observed in experiments, suggesting also new possibilities for experimental investigation.;2. Convective mass transfer across fluid interfaces in straight angular pores. Steady convective mass transfer to or from fluid interfaces in pores of angular cross-section is theoretically investigated. The model incorporates the essential physics of capillarity and solute mass transfer by convection and diffusion in corner fluid filaments. The geometry of the corner filaments, characterized by the fluid-fluid contact angle, the corner half-angle and the interface meniscus curvature, is accounted for. Boundary conditions of zero surface shear ('perfect-slip') and infinite surface shear ('noslip') at the fluid-fluid interface are considered. The governing equations for laminar flow within the corner filament and convective diffusion to or from the fluid-fluid interface are solved using finite-element methods. Flow computations are verified by comparing the dimensionless resistance factor and hydraulic conductance of corner filaments against recent numerical solutions by Patzek and Kristensen [2001]. Novel results are obtained for the average effluent concentration as a function of flow geometry and pore-scale Peclet number. These results are correlated to a characteristic corner length and local pore-scale Peclet number using empirical equations appropriate for implementation in pore network models. Finally, a previously published "2D-slit" approximation to the problem at hand is checked and found to be in considerable error.;3. Bubble evolution driven by solute diffusion during the process of supersaturated carbonated water flooding. In situ bubble growth in porous media is simulated using a pore network model that idealizes the pore space as a lattice of cubic chambers connected by square tubes. Evolution of the gas phase from nucleation sites is driven by the solute mass transfer from the flowing supersaturated water solution to the bubble clusters. Effects of viscous aqueous phase flow and convective diffusion in pore corners are explicitly accounted for. Growth of bubble clusters is characterised by a pattern of quasi-static drainage and fingering in the gas phase, an invasion percolation process controlled by capillary and gravitational forces. A stepwise solution procedure is followed to determine the aqueous flow field and the solute concentration field in the model by solving the conservation equations. Mobilization of bubbles driven by buoyancy forces is also studied. Results of bubble growth pattern, relative permeability and macroscopic mass transfer coefficient are obtained under different gas saturations and aqueous flow conditions.
机译:这项研究解决了许多有关多孔介质中流体对流传质的基本问题。考虑到(i)缓缓溶解在角孔或喉咙角中的湿性非水相液体(NAPL)的液体细丝的溶解以及(ii)气泡的命运在多孔介质中过饱和水相流动过程中产生的; 1。 NAPL膜的稳定性对润湿NAPL溶解的影响。润湿性深刻影响自然土壤中残留的NAPL污染物的分布。在优先的NAPL润湿性条件下,NAPL会保留在小孔中,并沿着孔壁的拐角和缝隙以厚膜(液体细丝)的形式保留。孔角处的NAPL膜可在NAPL填充的孔之间提供毛细管连续性,从而通过对流和扩散显着影响NAPL溶解到流动的水相中的行为。建立了孔隙网络模型,以研究润湿的NAPL在多孔介质中的溶解行为。使用模拟器研究了初始NAPL分布和NAPL膜稳定性对溶解行为的影响。由于NAPL膜的破裂,NAPL相失去了连续性,并分裂成不连续的NAPL填充孔簇。准状态排水和指状水相进入NAPL填充的孔隙被视为一种渗流渗滤过程,并采用分步程序求解流场和溶质浓度场。事实证明,NAPL膜的稳定性会严重影响传质速率,因此稳定的NAPL膜可提供更快的溶出度。网络模拟器再现了润湿NAPL在多孔介质中溶解的基本物理原理,并解释了实验中观察到的浓度-尾随行为,也为实验研究提供了新的可能性。2。对流传质穿过直角孔中的流体界面。从理论上研究了在对角横截面孔中流体对流或从流体界面的稳定对流传质。该模型结合了通过角流体丝中的对流和扩散产生的毛细管现象和溶质传质的基本物理原理。考虑了以流体-流体接触角,拐角半角和界面弯月面曲率为特征的拐角丝的几何形状。考虑了流体-流体界面处的零表面剪力(“完美滑移”)和无限表面剪力(“ noslip”)的边界条件。使用有限元方法求解角filament丝内的层流以及流体与流体界面之间的对流扩散的控制方程。通过将角丝的无量纲阻力因数和水力传导率与Patzek和Kristensen [2001]的最新数值解进行比较,验证了流量计算。获得了关于平均流出物浓度随流动几何形状和孔尺度佩克雷特数变化的新结果。使用适合于在孔网络模型中实施的经验方程,将这些结果与特征角长度和局部孔尺度皮克雷特数相关联。最后,检查先前针对手头问题发布的“ 2D狭缝”近似值,发现存在相当大的误差; 3。在过饱和碳酸水驱过程中,溶质扩散驱动气泡逸出。使用孔隙网络模型模拟多孔介质中的原位气泡生长,该模型将孔隙空间理想化为由方形管连接的立方室的格子。固相质量从流动的过饱和水溶液转移到气泡团簇,驱使气相从成核位置逸出。明确考虑了粘性水相流动和对流扩散在孔角处的影响。气泡簇的生长以气相中的准静态排水和指状为特征,其侵入渗透过程受毛细管力和重力控制。遵循逐步求解过程,通过求解守恒方程来确定模型中的水流场和溶质浓度场。还研究了由浮力驱动的气泡的动员。在不同的气体饱和度和水流条件下,获得了气泡生长模式,相对渗透率和宏观传质系数的结果。

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