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Flocculation and transport of cohesive sediment.

机译:凝聚性沉积物的絮凝和运输。

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摘要

An earlier model for floc dynamics utilizes a constant fractal dimension and a constant yield strength as a part of the model assumptions. However, several prior studies suggest that the fractal dimension of floc changes as floc size increases or decreases. Furthermore, the yield strength of floc is observed to be proportional to floc size and fractal dimension during breakup process. In this research, a variable fractal dimension is adopted to improve the previous flocculation model. Moreover, an equation for yield strength of floc is theoretically and mathematically derived. The newly derived equation is combined with flocculation models. By comparing with laboratory experiments on temporal evolution of floc size (mixing tank and Couette flow), this research demonstrates the importance of incorporating a variable fractal dimension and a variable floc yield strength into the model for floc dynamics. However, it still remains unclear as what are effects of variable fractal dimension and variable yield strength on the prediction of cohesive sediment transport dynamics. The second goal of the present study is to further investigate roles of floc dynamics in determining the predicted sediment dynamics in a tide-dominated environment. A 1DV numerical model for fine sediment transport is revised to incorporate four different modules for flocculation, i.e., no floc dynamics, floc dynamics with assumptions of constant fractal dimension and yield strength, floc dynamics for variable fractal dimensional only, and floc dynamics for considering both fractal dimension and yield strength variables. Model results are compared with measured sediment concentration and velocity time series at the Ems/Dollard estuary. Numerical model predicts very small (or nearly zero) sediment concentration during slack tide when floc dynamics is neglected or incorporated incompletely. This feature is inconsistent with the observation. When considering variable fractal dimension and variable yield strength in the flocculation model, numerical model predicts much smaller floc settling velocity during slack tide and hence is able to predict measured concentration reasonably well. Model results further suggest that, when sediment concentration is greater than about 0.1 g/l, there exists a power law relationship between mass concentration and settling velocity except very near the bed where turbulent shear is strong. This observation is consistent with earlier laboratory and field experiment on floc settling velocity. It is concluded that a complete floc dynamics formulation is important to modeling cohesive sediment transport. (Full text of this dissertation may be available via the University of Florida Libraries web site. Please check http://www.uflib.ufl.edu/etd.html)
机译:早期的絮体动力学模型利用恒定的分形维数和恒定的屈服强度作为模型假设的一部分。但是,一些先前的研究表明,絮凝物的分形维数随絮凝物尺寸的增加或减小而变化。此外,在破碎过程中,絮凝物的屈服强度与絮凝物的大小和分形维数成正比。在这项研究中,采用可变的分形维数来改进以前的絮凝模型。此外,从理论和数学上推导了絮凝体的屈服强度方程。新推导的方程式与絮凝模型结合在一起。通过与絮体尺寸(混合罐和库埃特流量)随时间变化的实验室实验进行比较,这项研究表明将可变的分形维数和可变的絮体屈服强度纳入絮体动力学模型的重要性。然而,由于分形维数和屈服强度的变化对内聚性泥沙运移动力学的预测有什么影响,目前还不清楚。本研究的第二个目标是进一步研究絮凝动力学在确定以潮汐为主的环境中预测的沉积物动力学中的作用。修改了1DV精细泥沙运移的数值模型,以纳入四个不同的絮凝模块,即无絮凝动力学,假定分形维数和屈服强度恒定的絮凝动力学,仅针对可变分形维数的絮凝动力学以及同时考虑这两者的絮凝动力学分形维数和屈服强度变量。将模型结果与在Ems / Dollard河口测得的泥沙浓度和速度时间序列进行比较。数值模型预测,当絮体动力学被忽略或不完全整合时,在退潮期间沉积物的浓度很小(或几乎为零)。此功能与观察结果不一致。当在絮凝模型中考虑可变的分形维数和可变的屈服强度时,数值模型预测在松弛潮期间絮凝物沉降速度要小得多,因此能够合理地预测测得的浓度。模型结果进一步表明,当沉积物浓度大于约0.1 g / l时,质量浓度与沉降速度之间存在幂律关系,除了非常靠近湍流剪切强的床附近。该观察结果与早期的絮凝沉降速度实验室和野外实验一致。结论是,完整的絮凝动力学公式对于内聚性泥沙运移建模非常重要。 (可通过佛罗里达大学图书馆网站获得本文的全文。请检查http://www.uflib.ufl.edu/etd.html)

著录项

  • 作者

    Son, Minwoo.;

  • 作者单位

    University of Florida.;

  • 授予单位 University of Florida.;
  • 学科 Engineering Geological.;Sedimentary Geology.;Engineering Civil.
  • 学位 Ph.D.
  • 年度 2009
  • 页码 190 p.
  • 总页数 190
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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