Hydraulic Geometry Brian Bledsoe Department of Civil Engineering Colorado State University.

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Presentation transcript:

Hydraulic Geometry Brian Bledsoe Department of Civil Engineering Colorado State University

Regime Theory / Hydraulic Geometry (e.g. Lacey 1929, Leopold and Maddock 1953) Channel parameters may be sufficiently described with power functions utilizing Q as the sole independent variable

Hydraulic Geometry - Exponents At-a-StationDownstream b is width, f is depth, and m is velocity

Downstream hydraulic geometry

The Basic Issue Predicting channel width / depth in the context of heterogeneous bed and bank conditions w, h, S, v Continuity Friction loss Sediment transport or incipient motion ???

Three General Approaches Empirical Regime Equations / Hydraulic Geometry Lacey, Simons and Albertson, Blench, USACE, Julien and Wargadalem, many others including “regional curves” Context-specific - require judgment / caution “Rational / Analytical” Copeland Method (now in HEC-RAS) Lateral Momentum Transfer - Parker Millar Extremal / Variational / Thermodynamic Minimum S, VS, Fr, dVS/dw Maximum f, Qs, Qs/S

Hydraulic Geometry Approach in Stable Channel Design Rooted in regime theory of Anglo-Indian engineers Canal design Low sediment loads Low variability in Q Does not directly consider sediment load (slope equations are dangerous for sand bed channels) Neglects energy principles and time scales of different adjustment directions Fluvial system is actually discontinuous, e.g. tributaries, variability in coefficients

Downstream hydraulic geometry equations for width provide an important channel design and analysis tool Depth, velocity, and slope equations are less reliable

Some Factors Affecting a Vegetation / soils / light interactions Root reinforcement and depth / bank height Woody debris inputs and bank roughness Bank cohesion / stratigraphy / drainage Freeze / thaw Sediment load Flow regime (e.g. elevation of veg. on banks) Return period of extremes vs. recovery time Lateral vs. vertical adjustability / time Historical context

Downstream Hydraulic Geometry and Boundary Sediments Schumm (1960) Richards (1982)

Hey and Thorne (1986) All Veg. Types

Hey and Thorne (1986) Separate Veg. Types

Downstream Hydraulic Geometry and Vegetation Hey and Thorne (1986) Grassy banks  a = % tree / shrub  a = % tree / shrub  a = 2.73 > 50% tree / shrub  a = 2.34 Andrews (1984) Thin  a = 4.3 Thick  a = 3.6

Hey and Thorne (1986) and Charlton et al. (1978) data

Davies-Colley (1997) and Hession et al. (2003) data

Log Watershed Area Log Channel Width Forest Grass km 2

% Silt and Clay Root Density (ml l -1 )

Values of a in w = aQ 0.5 Unit System Very Wide Average Width Very Narrow English SI Vegetation Density, Stiffness, Root Reinforcement Bank Cohesion Suspended Sediment Load Bed Material Size / Braiding Risk ?

Summary u Downstream hydraulic geometry relationships for width can provide a useful, additional relationship in channel design u Selection of the coefficient a is complicated and requires consideration of many factors u Vegetation effects tend to override sedimentary effects u Processes are scale-dependent?