Fritz R. Fiedler University of Idaho Department of Civil Engineering Simulation of Shallow Discontinuous Flow over Complex Infiltrating Terrain
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
What is complex terrain? Topography with characteristic length scales (amplitude and wavelength) similar to flow depth o two-dimensional flow
Examples Flooding o inundation mapping o dam breaks Overland Flow o hydraulics o hydrologic response Wetlands and Estuaries, and Tidal Flats
Physical Objectives Determine how Dynamic Surface Interactions affect Hydrologic Response Evaluate the Effects of Grazing – degenerates plant community changes infiltration changes microtopography
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
CPER
Outline Field Measurements Mathematical Model Results
Infiltration Measurements Disc infiltrometers Light- and heavy-grazed areas Bare and vegetated
Infiltration Variability High K vegetated (locally high elevation) Low K bare (locally low elevation)
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
Ground Microtopography
Shaded Relief Map
Mathematical Modeling Infiltration spatial variability (G-A model) Microtopography (2-D dynamic equations) Uniform rainfall Simplified flow resistance
Surface Water Equations
Numerical Challenges Non-linear hyperbolic system Strong source terms (sometimes “stiff”) Small depths / dry areas (discontinuous) Large gradients in dependent variables
Vector Form
Basic MacCormack Scheme Lx1 Operator :
Friction Slope: Point-Implicit Treatment
Convective Acceleration Upwinding
Smoothing Function
Lateral Inflow
ponded:
not ponded:
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
Comparative Numerical Examples Steady state kinematic wave solution (analytical) Dam break problem (analytical) Published results Iwagaki, 1955 (experimental) Woolhiser et al., 1996 (characteristics- based)
Dam Break Problem
Microtopographic Surface
Overland Flow Depths
Flow Depths and Velocity
Spatial Distribution of Infiltration Parameters
Flow Channels
Overland Flow Depths
Cumulative Infiltration
Simulated vs. Measured
Simulated Grazing Effects
Spatial Distribution of Reynolds Number and log(f )
Cross-Sectional Mean Reynolds Number vs. Friction Factor
Distribution of log(K S )
Plane Slope, Variable Ks
Mean Depth vs Discharge Variable K S
Effect of Microtopographic Amplitude
Mean Depth vs Discharge Variable Microtopography
Conclusions Plane approximation gross distortion Vegetation controls response Average/effective K not applicable Interactive infiltration important Reynolds No. - Friction Factor K-W assumption
Watch Your Step!