2008
DOI: 10.1007/s10596-008-9085-y
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A continuous/discontinuous Galerkin framework for modeling coupled subsurface and surface water flow

Abstract: We consider conjunctive surface-subsurface flow modeling, where surface water flow is described by the shallow water equations and ground water flow by Richards' equation for the vadose zone. Coupling between the models is based on the continuity of flux and water pressure. Numerical approximation of the coupled model using the framework of discontinuous Galerkin (DG) methods is formulated. In the subsurface, the local discontinuous Galerkin (LDG) method is used to approximate ground water velocity and hydraul… Show more

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Cited by 35 publications
(29 citation statements)
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“…In the hydrologic sciences, the development has been mainly concerned with relaxing the upper boundary condition at the land surface, which was treated traditionally as simple flux and operational surface water boundary (see review by Ebel et al, 2009). Advancements include fully coupled groundwater–surface water models (VanderKwaak and Loague, 2001; Panday and Huyakorn, 2004; Kollet and Maxwell, 2008; Dawson, 2008; Sulis et al, 2010); incorporation of land surface processes such as evaporation from bare soil and transpiration by plants (Kollet and Maxwell, 2008); and full mass, energy and momentum exchange with the atmosphere via coupled land surface models. On the other hand, in atmospheric sciences, major advancements have focused on improving the lower boundary condition (i.e., the subsurface), which was treated traditionally as simple box or force restore models covering only the top soil layers and ignoring the deeper subsurface and groundwater dynamics.…”
Section: Coupled Modeling Of Soil–vegetation–atmosphere Systemsmentioning
confidence: 99%
“…In the hydrologic sciences, the development has been mainly concerned with relaxing the upper boundary condition at the land surface, which was treated traditionally as simple flux and operational surface water boundary (see review by Ebel et al, 2009). Advancements include fully coupled groundwater–surface water models (VanderKwaak and Loague, 2001; Panday and Huyakorn, 2004; Kollet and Maxwell, 2008; Dawson, 2008; Sulis et al, 2010); incorporation of land surface processes such as evaporation from bare soil and transpiration by plants (Kollet and Maxwell, 2008); and full mass, energy and momentum exchange with the atmosphere via coupled land surface models. On the other hand, in atmospheric sciences, major advancements have focused on improving the lower boundary condition (i.e., the subsurface), which was treated traditionally as simple box or force restore models covering only the top soil layers and ignoring the deeper subsurface and groundwater dynamics.…”
Section: Coupled Modeling Of Soil–vegetation–atmosphere Systemsmentioning
confidence: 99%
“…A thorough review of the approaches used in coupled surface water–groundwater models is given by Ebel et al [2009]. The two most commonly used techniques are (1) first‐order exchange coefficient coupling [e.g., VanderKwaak , 1999; Panday and Huyakorn , 2004; Therrien et al , 2005; Ebel et al , 2009] and (2) specifying surface‐subsurface continuity of pressure and flux boundary conditions [e.g., Kollet and Maxwell , 2006; Maxwell and Kollet , 2008b; Dawson , 2008]. Even though approaches differ, all these models use a rigorous, physically based mathematical treatment of integrated surface‐subsurface flow [ Maxwell , 2009].…”
Section: Introductionmentioning
confidence: 99%
“…In this case, the porous medium model typically includes multiphase Darcy's law (Helmig 1997) that represents flows of several fluids or Richards' equation (1931) that describes movement of only water through saturated/unsaturated porous media. Coupling of subsurface flows described by the Richards equation and overland flows has been studied recently (Dawson 2008;Rybak et al 2015;Kollet and Maxwell 2006;Sulis et al 2010;Sochala et al 2009;Berninger et al 2014;Mosthaf et al 2011).…”
Section: Introductionmentioning
confidence: 99%