Abstract

We propose a one-dimensional Saint-Venant (open-channel) model for overland flows, including a water input–output source term modeling recharge via rainfall and infiltration (or exfiltration). We derive the model via asymptotic reduction from the two-dimensional Navier–Stokes equations under the shallow water assumption, with boundary conditions including recharge via ground infiltration and runoff. This new model recovers existing models as special cases, and adds more scope by adding water-mixing friction terms that depend on the rate of water recharge. We propose a novel entropy function and its flux, which are useful in validating the model’s conservation or dissipation properties. Based on this entropy function, we propose a finite volume scheme extending a class of kinetic schemes and provide numerical comparisons with respect to the newly introduced mixing friction coefficient. We also provide a comparison with experimental data.

Highlights

  • In quantifying the dynamics of a watercourse, the most important components of the hydrologic recharge and loss are the precipitation and infiltration processes, respectively

  • For the specific problem of modeling flooding caused by precipitation, the inclusion of a source term corresponding in published maps and institutional to the recharge or infiltration in the Saint-Venant system turns it from a conservation affiliations

  • Our aim is to construct a mathematical model for overland flows that is consistent with the physical phenomena that can affect the motion of such water

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Summary

Introduction

In quantifying the dynamics of a watercourse, the most important components of the hydrologic recharge and loss are the precipitation and infiltration processes, respectively These are important today in understanding and forecasting the impact of climate variability on the human and natural environment. Our goal in this paper is to derive a model akin to (1) via vertical averaging under the shallow water assumption, starting from the Navier–Stokes equations with a permeable Navier boundary condition to account for the infiltration and a kinematic boundary condition to consider the precipitation. We will see below that these friction terms are necessary to avoid paradoxical outcomes, such as perpetual motion, and, for simplicity, we will assume in this paper the most basic constitutive relations for this friction: linear in R for k+(R) and piecewise linear in I for k−(I), in agreement with approximations based on experimental results [3,17]. A C and C++ implementation of this code written by Matthieu Besson, Omar Lakkis, and Philip Townsend is freely available on request (an older version is given by [20])

Navier–Stokes Equations with Infiltration and Recharge
Geometric Set-Up and the Two-Dimensional Navier—Stokes Equations
The Wet Boundary
The Free Surface
Mixing Friction
Saint-Venant System with Recharge via Vertical Averaging
Dimensionless Navier–Stokes Equations
First-Order Approximation of the Dimensionless Navier–Stokes Equations
The Saint-Venant System with Recharge
Why the Mixing Friction?
Entropy
The Numerical Model
Well-Balanced Schemes
Kinetic Function
Kinetic Connection to Saint-Venant
Discretization and Kinetic Fluxes
Numerical Tests
Comparison with Real-World Data
Single-Level and Three-Level Cascades
Conclusions
Full Text
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