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Relaxation and reversibility of extended Taylor dispersion from a Markovian-Lagrangian point of view

机译:从马尔可夫-拉格朗日角度看泰勒扩展色散的弛豫和可逆性

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摘要

Taylor dispersion in a two-dimensional (2D) stratified velocity field describes a transition, called relaxation, from convective behaviour for short times, towards Fickian behaviour for large times and is partially reversible upon reversal of the flow direction. In 2D the physics are assumed to be governed by the unidirectional convection diffusion equation (2D uCDE). The approximate height-averaged 1D Generalised Telegraph Equation (GTE) catches an essential part of the longitudinal spreading. Contrary to the 1D Fickian approach, it explicitly accounts for the transient reversible nature [Camacho J. Purely global model for Taylor dispersion. Phys Rev E 1993/2;48(1); Berentsen CWJ, Verlaan ML, van Kruijsdijk CPJW. Upscaling and reversibility of Taylor dispersion in heterogeneous porous media. Phys Rev E 2005;71:046308]. Here we approach Taylor dispersion from a Lagrangian-Markovian point of view. In the redistribution model (RM) that we present, the Euler forward method accounts for convection and a probability redistribution matrix generates the transverse movement by diffusion over time. We consider two redistribution matrices. The first results from the direct discretisation of the Gaussian distribution function associated with the transverse mixing of the 2D uCDE. The resulting Gaussian redistribution model (GRM) is able to capture the multi-scale relaxation and reversibility behaviour of the full 2D uCDE. The correlated redistribution model (CRM) is the RM model with a redistribution matrix based on auto-correlation. The CRM is a generalisation of the correlated random walk model of [Scheideg-ger AE. The random walk model with auto-correlation of flow through porous media, Can J Phys 1958;36]. For uniform auto-correlation, the CRM model approximates the multi-scale relaxation nature of the 2D uCDE as a single scale relaxation process similar to the GTE. Moreover, it has the same variance as the GTE in the limit of the time step over relaxation time ratio to zero. For specific conditions the equality of the CRM model and the GTE is proven up to △t~2 order accuracy.
机译:二维(2D)分层速度场中的泰勒色散描述了从短时间的对流行为到大时间的Fickian行为的过渡(称为松弛),并且在流动方向逆转时可以部分逆转。在2D中,假设物理受单向对流扩散方程(2D uCDE)控制。高度平均的近似一维广义电报方程(GTE)捕获了纵向扩展的重要部分。与1D Fickian方法相反,它明确地说明了瞬态可逆性[Camacho J. Taylor色散的纯全局模型。 Phys Rev E 1993/2; 48(1);贝伦森(Berentsen)CWJ,韦拉(Verlaan ML),范·克鲁伊斯迪克(van Kruijsdijk)CPJW。异质多孔介质中泰勒分散的放大和可逆性。 Phys Rev E 2005; 71:046308]。在这里,我们从拉格朗日-马尔可夫观点出发,研究泰勒色散。在我们提出的再分配模型(RM)中,欧拉正向方法说明了对流,而概率再分配矩阵通过随时间的扩散生成横向运动。我们考虑两个重新分配矩阵。第一个结果是与2D uCDE的横向混合相关的高斯分布函数的直接离散化。所得的高斯再分配模型(GRM)能够捕获完整2D uCDE的多尺度松弛和可逆行为。相关的再分配模型(CRM)是具有基于自相关的再分配矩阵的RM模型。 CRM是对[Scheideg-ger AE的相关随机游走模型的概括。具有通过多孔介质的流量自相关的随机游走模型,Can J Phys 1958; 36]。对于统一的自相关,CRM模型将二维uCDE的多尺度弛豫特性近似为类似于GTE的单尺度弛豫过程。而且,它在松弛时间比为零的时间步长极限中具有与GTE相同的方差。对于特定条件,CRM模型和GTE的相等性被证明达到△t〜2阶精度。

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