Abstract
To begin a rising-head permeability test in a monitoring well (MW), the water level is lowered in the pipe. If it is lowered down to the screen, the recovery graph may differ from the theoretical straight line, making it difficult to assess the mean field hydraulic conductivity. A numerical analysis (finite element method) of this type of test, considering the complete equations for saturated and unsaturated flow, is presented. The numerically obtained graphs are similar to those of real field tests. In an aquitard, when the filter pack is made of fine sand, which retains water by capillarity, the screen dewatering influence is hardly visible in the velocity graph and is undetected in the usual semilog graph. In an aquitard, when the filter pack cannot retain water by capillarity during dewatering, the semilog graph presents two straight-line portions. The velocity graph, a representation of the conservation equation, helps to distinguish the early time interval, when the groundwater fills the screen and the filter pack, and the later interval, when it fills only the pipe. The later portion of the graph must be used to calculate the hydraulic conductivity. In an unconfined aquifer, when there is no filter pack, dewatering down to the screen by pumping significantly lowers the water table around the MW. The usual semilog graph appears as a set of two straight lines. The velocity graph indicates that all calculations must consider a piezometric level that is lower than that measured before dewatering. In all cases, the velocity graph shows clearly what happened during the numerically simulated tests. The more complex case of an MW installed with a filter pack in an unconfined aquifer and tested using a mechanical slug was not numerically examined in this paper.Key words: hydraulic conductivity, rising head, monitoring well, numerical analysis.
Publisher
Canadian Science Publishing
Subject
Civil and Structural Engineering,Geotechnical Engineering and Engineering Geology
Cited by
18 articles.
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