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Development and Testing of a Surface-Water Flow Model for Shark River Slough

Poster presented December 2000, at the Greater Everglades Ecosystem Restoration Conference

James E. Saiers1, Carl H. Bolster1, Thomas J. Smith2

1School of Forestry, Yale University, New Haven, CT
2USGS-BRD, Miami, FL

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1. Abstract

In the work reported here, we develop a two-dimensional diffusion model for surface-water movement, and we test this model against hydrologic data collected from the Shark River Slough of the Florida Everglades. The equations that govern the model are derived under the assumptions that surface-water flow is laminar and that a power-law relationship quantifies the dependence of flow velocity on water depth. We simplify the model formulation by assuming uniform rates of evapotranspiration, a constant ground-surface slope, and spatially homogeneous vegetative cover. In both inverse and predictive simulations, model calculations closely match surface-water stages measured over a 27-km transect within the slough.

2. Objectives

3. Site Description

The Shark River Slough serves as the primary means of delivery of freshwater from Water Conservation Areas 3A and 3B to the Florida Bay and the Gulf of Mexico (see site map). Sawgrass and spikerush, interspersed with dry tree islands, represent the dominant vegetation types within the slough. The central part of the slough is underlain with organic muck, which, in turn, is underlain by limestone. Depth of water in the slough is on the order of a meter or less. Water quality measurements made at site S1 for a one-year period beginning in October 1997 reveal that surface-water concentrations of total dissolved solids range from 60 mg/L to 350 mg/L.
Illustration of Site Map
[larger image]

4. Model Development

The model is based on the nonlinear diffusion equation, which is derived by combining the appropriate forms of the continuity and the momentum equations. In two-dimensional form, the nonlinear diffusion equation can be expressed as

nonlinear diffusion equation (1)

where h is hydraulic head, Sy is specific yield, Kf is the surface-water conductivity coefficient, d is water depth, beta is an exponential constant, E is the evapotranspiration rate, and P is precipitation rate. Equation (1) is derived by assuming that the inertial and acceleration terms of the momentum equations are negligible and by assuming that overland flow velocity can be expressed as a power function of water depth. We solved the diffusion equation using a finite-difference method with a predictor-corrector time-stepping scheme.

5. Model Domain

6. Sequence of Simulations

7. Model Calibration

Graph showing model calibration data, as measured at P33
Graph showing model calibration data, as measured at P36
Graph showing model calibration data, as measured at S1

Model-calculated hydraulic heads (solid lines) closely reproduce measured heads (symbols) for the calibration period. Best-fit values of Kf and beta are 6.18 x 106 m0.6 d-1 and 0.439, respectively. The dashed lines represent rainfall rates, as measured at P33, P35, and P36, and the heavy line near the bottom of each plot represents evapotranspiration rates, measured at P33.

8. Model Prediction

Graph showing model prediction data for P33
Graph showing model prediction data for P36
Graph showing model prediction data for S1

Using the best-fit values of Kf and beta determined from from calibration, the model predicts both the spatial and temporal variations in head along the 27-km long transect with good success.

9. Conclusions

Our model is based on several simplifying assumptions, which are necessary given the lack of data on the spatial distribution in wetland properties and vertical fluxes of water. The key assumptions of the model are that (1) evapotranspiration rates are uniform throughout the domain, (2) variability in rainfall rates can be described with a three-zone discretization, (3) exchanges of water between the surface and subsurface are negligible, (4) the ground-surface slope is uniform, and (5) the frictional resistance parameters (i.e., Kf and beta) are constant in time and space. When taken in context to these assumptions, our results suggest that accurate predictions of surface-water flow for extended times and over long distances can be accomplished without extensive characterization of the the spatial variability in the source-sink terms and by treating the physical properties of the wetland as homogeneous.

10. Acknowledgments

This research was supported in significant part by DOI's Critical Ecosystem Studies Initiative, a special funding initiative for Everglades restoration administered by the National Park Service; and in part by USGS's Florida Caribbean Science Center. We thank Gordon Anderson, Ed German, and Kevin Kotun for providing us with access to data on rainfall, evapotranspiration, and surface-water levels.


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