王文学, 郝清扬, 薛景元, 姜彤, 董金玉. 含水层底部单孔非完整疏放水井渗流特征砂槽试验[J]. 煤炭学报, 2023, 48(3): 1290-1301.
引用本文: 王文学, 郝清扬, 薛景元, 姜彤, 董金玉. 含水层底部单孔非完整疏放水井渗流特征砂槽试验[J]. 煤炭学报, 2023, 48(3): 1290-1301.
WANG Wenxue, HAO Qingyang, XUE Jingyuan, JIANG Tong, DONG Jinyu. Sand tank test on seepage characteristics of a single partially penetrating de-watering well from the bottom of an overlying aquifer[J]. Journal of China Coal Society, 2023, 48(3): 1290-1301.
Citation: WANG Wenxue, HAO Qingyang, XUE Jingyuan, JIANG Tong, DONG Jinyu. Sand tank test on seepage characteristics of a single partially penetrating de-watering well from the bottom of an overlying aquifer[J]. Journal of China Coal Society, 2023, 48(3): 1290-1301.

含水层底部单孔非完整疏放水井渗流特征砂槽试验

Sand tank test on seepage characteristics of a single partially penetrating de-watering well from the bottom of an overlying aquifer

  • 摘要: 为研究含水层底部疏放水井渗流特征,设计研发了一种60°扇形体渗流砂槽系统,以潜水含水层底部疏放水为例,开展了不同井长单井非完整井疏放水渗流砂槽试验,研究结果表明:疏放水引起浸润线的下降,并在其上方形成饱和毛细水带负压区;疏放水过程中含水层底部非完整井上部可划分为上层毛细水带、支持毛细水带、饱和毛细水带及自由水饱和带,饱和毛细水带可有效阻止上部空气进入井内;非完整井井片内部压力P存在4种水压分布形态,即P=0、P>0、P<0以及Pup<0且Pdown>0,根据井内压力及井片上部自由水饱和带、饱和毛细带的分布,含水层底部非完整井疏放水似稳定流态水压分布可概化7种模型;非满管段的形成导致其上部自由水压力不能连续传递,其分布不再是满管时的由下至上递减规律,当井片上方存在浸润线时,压力水头分布由下至上呈先增加后减小的规律;当井片上方存在自由水饱和带或较大范围的饱和毛细水带时,渗流量随井内压力减小而增加,当自由水饱和带消失且饱和毛细水带垂直分布较小时,井内压力的减小对渗流的增加效应不明显;非完整井井长的增加可有效增加渗流量,但当井长大于临界值后,渗流量不再随着井长的增加而变化;疏放水过程中,疏放水量由静态补给与动态补给构成且静态补给以一阶指数函数减少、动态补给以一阶指数函数增加。

     

    Abstract: In order to study the seepage characteristics of dewatering from an aquifer bottom, a sand tank system was designed with the cross section being a sector of 60°,and the dewatering test from an unconfined aquifer bottom using partially penetrating dewatering wells with different well lengths was conducted. The results show that the phreatic line falls off with dewatering process, and a saturated capillary zone with negative pressure forms above it. The upper capillary zone, supporting capillary zone, saturated capillary zone and free water saturation zone can be formed above the dewatering well in aquifer, and the saturated capillary zone can effectively prevent the upper air from entering the well. The well inner pressure P includes four kinds of circumstances, which are P=0,P>0,P<0 and Pup<0 with Pdown>0,and the distribution of quasi-steady flow pressure distribution can be generalized into seven models based on well inner pressure, saturated capillary zone and free water saturation zone. The water pressure transfer of free water cannot be interrupted as the partly-filled well. The distribution of water pressure head is no longer decreasing from bottom to top in the fully filled well, but increases first and then decreases from bottom to top when a phreatic line is formed above the well. The seepage flow will increase with well inner pressure decrease if the saturated capillary zone and free water saturation zone present a wide distribution. When the free water saturation zone disappears and the saturated capillary zone presents a small range vertical distribution, the well inner pressure decrease plays less influence on seepage flow increase. The seepage flow increases with the well length increase, however, when the well length is greater than a critical length, the seepage flow no longer increases with well length increase. In the dewatering process, the seepage flow is composed of static and dynamic recharge, and the static recharge decreases with an exponential function, while the dynamic recharge increases with an exponential function.

     

/

返回文章
返回