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Dam sites in soluble rocks: a model of increasing leakage by dissolutional widening of fractures beneath a dam

机译:可溶性岩石中的坝位:通过坝下裂缝的溶出扩展扩大渗漏的模型

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Water flowing through narrow fissures and fractures in soluble rock, e.g. limestone and gypsum, widens these by chemical dissolution. This process, called karstification, sculptures subterranean river systems which drain most of their catchment. Close to dam sites, unnaturally high hydraulic gradients are present to drive the water impounded in the reservoir downstream through fractures reaching below the dam, Under such conditions, the natural process of karstification is accelerated to such an extent that high leakage rates may arise, which endanger the operation of the hydraulic structure. Model simulations of karstification below dams by coupling equations of dissolutional widening to hydrodynamic flow are presented. The model scenario is a dam 100 m wide in limestone or gypsum. The modelling domain is a two-dimensional slice 1 m wide directed perpendicular to the dam. It extends 375 m vertically and 750 m horizontally. The dam is located in its center. This domain is divided by fractures and fissures into blocks of 7.5 X 7.5 X 1 m. The average aperture width of the fractures is 0.02 cm. We performed model runs on standard scenarios for a dam site in limestone with the height H of impounded water 150 m, a horizontal impermeable apron of width W= 262 m and a grouting curtain reaching down to a depth of G =97 m. In a second scenario, we changed these construction features to G = 187 m and W= 82 m. To calculate widening of the fractures, well-established experimental data on the dissolution of limestone and gypsum have been used as they occur in such geochemical settings. All model runs show similar characteristic behaviour. Shortly after filling, the reservoir exhibits a small leakage of about 0.01 m~3 s~(-1), which increases steadily until a breakthrough event occurs after several decades with an abrupt increase of leakage to about 1 m~3 s~(-1) within the short time of a few years. Then, flow in the fractures becomes turbulent and the leakage increases to 10 m~3 s~(-1) in a further time span of about 10 years. The widths of the fractures are visualized in various time steps. Small channels propagate downstream and leakage rises slowly until the first channel reaches the surface downstream. Then breakthrough occurs, the laminar flow changes to turbulent and a dense net of fractures which carry flow is established. We performed a sensitivity analysis on the dependence of breakthrough times on various parameters, determining breakthrough. These are the height of impounded water H, the depth G of grouting, the average aperture width a_0 of the fractures and the chemical parameters, which are c_(eq) the equilibrium concentration of Ca with respect to calcite and the Ca-concentration c_(in) of the inflowing water. The results show that the most critical parameter is a_0. At fracture aperture widths of 0.01 cm, breakthrough times are above 500 years. For values of a_0>0.02 cm, however, breakthrough times are within the lifetime of the structure. We have also modelled dam sites in gypsum, which exhibit similar breakthrough times. However, after breakthrough, owing to the much larger dissolution rates of gypsum, the time until unbearable leakage is obtained, is only a few years. The modelling can be applied to complex geological settings, as phreatic cave conduits below the dam, or a complex stratigraphy with varying properties of the rock with respect to hydraulic conductivity and solubility. A few examples are given. In conclusion, our results support the assumption that increasing leakage of dam sites may be caused by dissolutional widening of fractures.
机译:水流过可溶岩石中的狭窄裂缝和裂缝,例如石灰石和石膏通过化学溶解来扩大它们。这个过程称为喀斯特地化作用,它雕刻出了大部分流域流失的地下河系。在大坝附近,存在非自然的高水力梯度,以驱使通过下游的裂缝将蓄积在水库下游的水运到大坝下方。在这种情况下,岩溶的自然过程被加速到一定程度,以至于可能产生高泄漏率,从而危害水工结构的运行。提出了通过溶胀加宽与水动力流耦合方程的坝下岩溶化模型模拟。模型场景是一个100 m宽的石灰石或石膏坝。建模域是一个垂直于大坝的1 m宽的二维切片。它垂直延伸375 m,水平延伸750 m。大坝位于其中心。该区域按裂缝和裂缝分为7.5 X 7.5 X 1 m的块。裂缝的平均孔径宽度为0.02 cm。我们在标准场景中对石灰岩中的坝址进行了模型运行,蓄水的高度H为150 m,宽度为W = 262 m的水平防渗围裙,并且灌浆幕布的深度达到G = 97 m。在第二种情况下,我们将这些构造特征更改为G = 187 m和W = 82 m。为了计算裂缝的扩展,已使用关于石灰石和石膏溶解的公认实验数据,因为它们发生在这种地球化学环境中。所有模型运​​行均显示相似的特征行为。注入后不久,储层出现约0.01 m〜3 s〜(-1)的小泄漏,并稳定增加,直到几十年后发生突破事件,泄漏突然增加到约1 m〜3 s〜(- 1)在短短的几年内。然后,在大约10年的时间内,裂缝中的流动变得湍流,泄漏增加到10 m〜3 s〜(-1)。在不同的时间步长中可以看到裂缝的宽度。小通道向下游传播,泄漏缓慢上升,直到第一个通道到达下游表面。然后发生突破,层流变为湍流,并建立了一个致密的裂缝网来承载流量。我们根据击穿时间对各种参数的依赖性进行了敏感性分析,确定了击穿。这些是注入水的高度H,注浆深度G,裂缝的平均孔径宽度a_0和化学参数,它们是Ca相对于方解石的平衡浓度和Ca浓度c_(eq)。在)流入的水。结果表明,最关键的参数是a_0。在缝隙孔宽度为0.01 cm时,突破时间超过500年。但是,对于a_0> 0.02 cm的值,穿透时间在结构寿命内。我们还对石膏中的坝址进行了建模,它们具有相似的突破时间。但是,在突破之后,由于石膏的溶解速率大得多,直到获得难以忍受的泄漏为止的时间只有几年。该模型可以应用于复杂的地质环境,例如位于大坝下方的潜水洞导管,或者具有复杂的地层,岩石在水力传导率和溶解度方面具有变化的特性。举几个例子。总之,我们的结果支持这样的假设,即坝体渗漏增加可能是由于裂缝的溶解性扩展所致。

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