Please use this identifier to cite or link to this item: https://doi.org/10.1016/S0309-1708(98)00038-4
DC FieldValue
dc.titleAnalysis of continuous and pulsed pumping of a phreatic aquifer
dc.contributor.authorZhang, H.
dc.contributor.authorBaray, D.A.
dc.contributor.authorHocking, G.C.
dc.date.accessioned2014-06-17T08:13:23Z
dc.date.available2014-06-17T08:13:23Z
dc.date.issued1999-02-24
dc.identifier.citationZhang, H., Baray, D.A., Hocking, G.C. (1999-02-24). Analysis of continuous and pulsed pumping of a phreatic aquifer. Advances in Water Resources 22 (6) : 623-632. ScholarBank@NUS Repository. https://doi.org/10.1016/S0309-1708(98)00038-4
dc.identifier.issn03091708
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/65133
dc.description.abstractIn a phreatic aquifer, fresh water is withdrawn by pumping from a recovery well. As is the case here, the interfacial surface (air/water) is typically assumed to be a sharp boundary between the regions occupied by each fluid. The pumping efficiency depends on the method by which the fluid is withdrawn. We consider the efficiency of both continuous and pulsed pumping. The maximum steady pumping rate, above which the undesired fluid will break through into the well, is defined as critical pumping rate. This critical rate can be determined analytically using an existing solution based on the hodograph method, while a Boundary Element Method is applied to examine a high flow rate, pulsed pumping strategy in an attempt to achieve more rapid withdrawal. A modified kinematic interface condition, which incorporates the effect of capillarity, is used to simulate the fluid response of pumping. It is found that capillarity influences significantly the relationship between the pumping frequency and the fluid response. A Hele-Shaw model is set up for experimental verification of the analytical and numerical solutions in steady and unsteady cases for pumping of a phreatic aquifer. When capillarity is included in the numerical model, close agreement is found in the computed and observed phreatic surfaces. The same model without capillarity predicts the magnitude of the free surface fluctuation induced by the pulsed pumping, although the phase of the fluctuation is incorrect.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1016/S0309-1708(98)00038-4
dc.sourceScopus
dc.subjectCapillary fringe
dc.subjectFree surface
dc.subjectHele-Shaw model
dc.subjectPulsed pumping
dc.typeArticle
dc.contributor.departmentCIVIL ENGINEERING
dc.description.doi10.1016/S0309-1708(98)00038-4
dc.description.sourcetitleAdvances in Water Resources
dc.description.volume22
dc.description.issue6
dc.description.page623-632
dc.description.codenAWRED
dc.identifier.isiut000079211500007
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