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Fritz R. Fiedler University of Idaho Department of Civil Engineering Simulation of Shallow Discontinuous Flow over Complex Infiltrating Terrain
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What is shallow discontinuous flow? Shallow: depth << wavelength o vertical acceleration negligible o depth-averaged NS equations Discontinuous: both dry and wet areas o shocks o topographic control o infiltration variability
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What is complex terrain? Topography with characteristic length scales (amplitude and wavelength) similar to flow depth o two-dimensional flow
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Examples Flooding o inundation mapping o dam breaks Overland Flow o hydraulics o hydrologic response Wetlands and Estuaries, and Tidal Flats
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Physical Objectives Determine how Dynamic Surface Interactions affect Hydrologic Response Evaluate the Effects of Grazing – degenerates plant community changes infiltration changes microtopography
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Study Area Description Central Plains Experimental Rangeland Light- and heavy-grazed enclosures 1/2-hour, 100-year rain: ~100 mm/hr 1-hour, 100-year rain: ~75 mm/hr Patchy vegetation
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CPER
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Outline Field Measurements Mathematical Model Results
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Infiltration Measurements Disc infiltrometers Light- and heavy-grazed areas Bare and vegetated
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Infiltration Variability High K vegetated (locally high elevation) Low K bare (locally low elevation)
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Microtopography The ground surface topography with approximately the same order amplitude and frequency as the overland flow depth in a given situation: –related to rainfall intensity –related to infiltration characteristics –caused by vegetation growth
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Ground Microtopography
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Shaded Relief Map
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Mathematical Modeling Infiltration spatial variability (G-A model) Microtopography (2-D dynamic equations) Uniform rainfall Simplified flow resistance
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Surface Water Equations
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Numerical Challenges Non-linear hyperbolic system Strong source terms (sometimes “stiff”) Small depths / dry areas (discontinuous) Large gradients in dependent variables
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Vector Form
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Basic MacCormack Scheme Lx1 Operator :
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Friction Slope: Point-Implicit Treatment
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Convective Acceleration Upwinding
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Smoothing Function
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Lateral Inflow
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ponded:
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not ponded:
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High-performance computing Fortran Loop optimizations o most dependencies eliminated o unrolling, fusion o single-stride memory access Shared-memory parallel processing o PC environment
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Comparative Numerical Examples Steady state kinematic wave solution (analytical) Dam break problem (analytical) Published results Iwagaki, 1955 (experimental) Woolhiser et al., 1996 (characteristics- based)
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Dam Break Problem
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Microtopographic Surface
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Overland Flow Depths
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Flow Depths and Velocity
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Spatial Distribution of Infiltration Parameters
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Flow Channels
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Overland Flow Depths
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Cumulative Infiltration
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Simulated vs. Measured
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Simulated Grazing Effects
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Spatial Distribution of Reynolds Number and log(f )
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Cross-Sectional Mean Reynolds Number vs. Friction Factor
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Distribution of log(K S )
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Plane Slope, Variable Ks
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Mean Depth vs Discharge Variable K S
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Effect of Microtopographic Amplitude
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Mean Depth vs Discharge Variable Microtopography
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Conclusions Plane approximation gross distortion Vegetation controls response Average/effective K not applicable Interactive infiltration important Reynolds No. - Friction Factor K-W assumption
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Watch Your Step!
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