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Modelling the effects of porous media deformation on the propagation of water-table waves in a sandy unconfined aquifer

机译:模拟多孔介质变形对桑迪含水层中水台波传播的影响

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This paper examines the influence of porous media deformation on water-table wave dispersion in an unconfined aquifer using a numerical model which couples Richards' equation to the poro-elastic model. The study was motivated by the findings of Shoushtari et al. (J Hydrol 533:412-440, 2016) who were unable to reproduce the observed wave dispersion in their sand flume data with either numerical Richards' equation models (assuming rigid porous media) or existing analytic solutions. The water-table wave dispersion is quantified via the complex wave number extracted from the predicted amplitude and phase profiles. A sensitivity analysis was performed to establish the influence of the main parameters in the poro-elastic model, namely Young's modulus (E) and Poisson's ratio (nu). For a short oscillation period (T = 16.4 s), the phase lag increase rate (k (i)) is sensitive to the chosen values of E and nu, demonstrating an inverse relationship with both parameters. Changes in the amplitude decay rate (k (r)), however, were negligible. For a longer oscillation period (T = 908.6 s), variations in the values of E and nu resulted in only small changes in both k (r) and k (i). In both the short and long period cases, the poro-elastic model is unable to reproduce the observed wave dispersion in the existing laboratory data. Hence porous media deformation cannot explain the additional energy dissipation in the laboratory data. Shoushtari SMH, Cartwright N, Perrochet P, Nielsen P (2016) The effects of oscillation period on groundwater wave dispersion in a sandy unconfined aquifer: sand flume experiments and modelling. J Hydrol 533:412-440.
机译:本文研究了利用将Richards等式与Poro-Elastic模型的数值模型进行了多孔介质变形对非整合含水层的水台波分散的影响。该研究是由Shoushtari等人的研究结果的激励。 (J Waterold 533:412-440,2016)无法使用数值理查德的公式模型(假设刚性多孔介质)或现有的分析溶液在其砂水管数据中再现观察到的波形分散。通过从预测幅度和相位轮廓提取的复杂波数量化水表波分散。进行敏感性分析,以确定主要参数在浮标 - 弹性模型中的影响,即年轻的模量(e)和泊松比(nu)。对于短振荡周期(t = 16.4 s),相滞后增加率(k(i))对E和Nu的所选值敏感,展示了与两个参数的反向关系。然而,幅度衰减率的变化(k(r))可以忽略不计。对于更长的振荡周期(T = 908.6s),E和NU值的变化仅导致K(R)和K(I)的少量变化。在短期和长期的情况下,Poro-Elastic模型无法在现有实验室数据中再现观察到的波形分散。因此,多孔介质变形无法解释实验室数据中的额外节能。 Shoushtari SMH,Cartwright N,Perrochet P,Nielsen P(2016)振荡期对砂质非排水含水层地下水波分散的影响:砂水管实验和建模。 J Hydol 533:412-440。

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