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平流输运现象以更好地理解现场和建模实践中的弥散

Advective Transport Phenomena to Better Understand Dispersion in Field and Modeling Practice.

出版信息

Ground Water. 2020 Jan;58(1):46-55. doi: 10.1111/gwat.12883. Epub 2019 Apr 15.

DOI:10.1111/gwat.12883
PMID:30891733
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7004079/
Abstract

The absence of recent research on dispersion in engineering applications indicates the need for a description that is more focused on field and modeling practice. Engineers may benefit from simple calculation tools allowing them to understand the processes encountered in the field. Based on a conceptual model for advective transport through an elongated conductivity zone, for example, in fluvial sediments, explicit expressions are presented for macro-scale phenomena: (1) the different travel distances of water particles traveling in laminar flow through and adjacent to a single zone with conductivity higher or lower than that of the aquifer; (2) the affected thickness of the bundle of flowlines; (3) the distinction of inflow, outflow, and through-flow sections; (4) the development of a plume front vs. that of a tail; (5) conservation of mass causing water particles to travel both slower and faster than the aquifer average velocity while passing a single zone. The spread derived from a spatial distribution in a field experiment relates to the geometric mean of the spreads of the plume front and tail. The results obtained for a single conductivity zone are expanded for a general aquifer that is characterized by stochastic parameters. A fundamental new expression describes the dispersive mass flux as the product of the advective volume shift and the related local concentration difference. Contrary to Fickian theory, the dispersive mass flux in both the front and tail of a plume in highly heterogeneous aquifers is limited. In modeling, the advective volume shift is proportional to the cell size.

摘要

工程应用中弥散的研究缺乏表明需要一种更关注现场和建模实践的描述。工程师可能会受益于简单的计算工具,这些工具可以帮助他们理解在现场遇到的过程。例如,基于通过具有高于或低于含水层电导率的单个区域的平流输送的对流传输的概念模型,给出了宏观现象的显式表达式:(1) 在单个区域中通过和相邻处的层流中行进的水颗粒的不同行进距离,该区域的电导率高于或低于含水层;(2) 流线束的受影响厚度;(3) 入流、出流和贯穿流部分的区别;(4) 羽流前缘与尾流的发展;(5) 质量守恒导致水颗粒在穿过单个区域时比含水层平均速度慢和快。来自现场实验的空间分布的扩散与羽流前缘和尾流的扩散的几何平均值相关。对于单个电导率区域获得的结果被扩展到具有随机参数的一般含水层。基本的新表达式将弥散质量通量描述为对流体积转移和相关局部浓度差的乘积。与菲克理论相反,在高度非均质含水层中羽流的前缘和尾流中的弥散质量通量是有限的。在建模中,对流体积转移与单元尺寸成正比。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/5e237edcec72/GWAT-58-46-g007.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/90ea1870242b/GWAT-58-46-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/2a20092fc39f/GWAT-58-46-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/5e237edcec72/GWAT-58-46-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/57b7989615a0/GWAT-58-46-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/74825b9bfa67/GWAT-58-46-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/844b/7004079/58294cf06ce9/GWAT-58-46-g003.jpg
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