Revisit of advection-dispersion equation model with velocity-dependent dispersion in capturing tracer dynamics in single empty fractures
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王沐
[1
]
赵卫东
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机构:
School of Resources and Environmental Engineering, Hefei University of TechnologySchool of Resources and Environmental Engineering, Hefei University of Technology
赵卫东
[1
]
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Rhiannon Garrard
[2
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Yong Zhang
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Department of Geological Sciences, University of Alabama
College of Mechanics and Materials, Hohai UniversitySchool of Resources and Environmental Engineering, Hefei University of Technology
Yong Zhang
[2
,3
]
刘咏
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机构:
School of Food and Biotechnology Engineering, Hefei University of TechnologySchool of Resources and Environmental Engineering, Hefei University of Technology
刘咏
[4
]
钱家忠
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School of Resources and Environmental Engineering, Hefei University of TechnologySchool of Resources and Environmental Engineering, Hefei University of Technology
钱家忠
[1
]
机构:
[1] School of Resources and Environmental Engineering, Hefei University of Technology
[2] Department of Geological Sciences, University of Alabama
[3] College of Mechanics and Materials, Hohai University
[4] School of Food and Biotechnology Engineering, Hefei University of Technology
Dispersion coefficient;
molecular diffusion;
roughness;
variation trend;
single fracture;
D O I:
暂无
中图分类号:
P641.2 [地下水动力学];
学科分类号:
0818 ;
081803 ;
摘要:
An accurate quantification of the contaminant transport through fractured media is critical for dealing with water-quality related scientific and engineering issues, where the dispersion coefficient is an important and elusive parameter for the solute transport modeling. Many previous studies show that the dispersion coefficient(D) in the standard advection-dispersion equation(ADE) model can be approximated by D=avλ(where a is the dispersivity), a formula to be revisited systematically in this study by laboratory experiments and model analysis. First, a series of tracer transport experiments in single empty fractures are conducted in cases of different hydraulic gradients. Second, the tracer breakthrough curves are determined by simulations based on the ADE model, to obtain the dispersion coefficients corresponding to various fracture roughnesses and flow velocities. A varying trend of λ is analyzed under different flow conditions. Results show that although the standard ADE model cannot be used to characterize the late-time tailing of the tracer BTCs, likely due to the solute retention, this simple model can simulate most of the solute mass dynamics moving through fractures and may therefore provide information for estimating the dispersion in parsimonious models appropriate for the non-Fickian transport. The following three conclusions are drawn:(1) the peak of the breakthrough curves comes earlier with increasing the roughness, according to the ADE simulation,(2) the value of λ generally decreases as the relative roughness of the fracture increases,(3) the value of λ is approximately equal to 2.0 when the dispersion is dominated by the molecular diffusion in the smooth fracture.
机构:
Nanyang Normal Univ, Coll Math & Stat, Nanyang 473061, Henan, Peoples R ChinaNanyang Normal Univ, Coll Math & Stat, Nanyang 473061, Henan, Peoples R China
Wang, Shunqin
Sun, Chunlong
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Shandong Univ Technol, Inst Appl Math, Zibo 255049, Shandong, Peoples R ChinaNanyang Normal Univ, Coll Math & Stat, Nanyang 473061, Henan, Peoples R China
Sun, Chunlong
Li, Gongsheng
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Shandong Univ Technol, Inst Appl Math, Zibo 255049, Shandong, Peoples R ChinaNanyang Normal Univ, Coll Math & Stat, Nanyang 473061, Henan, Peoples R China
机构:
Japan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, JapanJapan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, Japan
Kurikami, Hiroshi
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Malins, Alex
Takeishi, Minoru
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Japan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, JapanJapan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, Japan
Takeishi, Minoru
Saito, Kimiaki
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Japan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 2-2-2 Uchisaiwai-cho, Chiyoda, Tokyo,100-8577, JapanJapan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, Japan
Saito, Kimiaki
Iijima, Kazuki
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Japan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, JapanJapan Atomic Energy Agency (JAEA), Sector of Fukushima Research and Development, 10-2 Fukasaku, Miharu-machi, Tamura-gun, Fukushima,963-7700, Japan