Conveyance Estimation System (CES) Launch

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1 (CES) Launch Conveyance Principles Caroline McGahey 10 June 2004

2 Why is there a new approach? Existing 1D software still based on historic hand-calculation methods - not based in rigorous physics - as SCM poor predictions for overbank flow - as DCM ignores lateral shearing - all physical processes lumped into one catch-all parameter - Manning n

3 Why is there a new approach? Research advances over past 20 years understanding flow mechanisms quantifying associated energy losses Quality data sets from: - experimental set-ups e.g. FCF - purpose-made river measurements - large scale rivers - EA gauging sites Advent of computing power enabled coding & testing of methods against extensive database

4 Energy transfer mechanisms 2. Momentum Transfer 2. Shear layer Direction of flow 1. Boundary shear stresses 3. Secondary flows

5 Meandering mechanisms

6 Observed flow features Ikeda et al 2001 Shiono & Muto 1998 Sellin 1964 Shiono & Muto 1998 Ikeda et al 2001

7 Meandering velocity profiles U d AA A A AA BB B B C BB C CC Distance across section

8 Conveyance calculation Depth integration of Reynolds-Averaged Navier-Stokes equations dy Integrate unit flow rate q (m 2 /s) Q = qdy 2 K = Q / S f 1

9 Conveyance calculation ghs o β f q 2 8H 2 + y λ H f q y q H = α Γ+ (1 α) y C uvq H 2 I II III IV V I II III IV V hydrostatic pressure boundary friction turbulence due to lateral shear straight secondary flow losses meandering secondary flow losses

10 Calibration coefficients Terms to cover all energy losses - coefficients for: - skin friction f based on RA unit roughness n l - lateral shearing - dimensionless eddy viscosity λ - straight secondary flow losses Γ - meandering secondary flow losses C uv Form loss is not accounted for

11 Calibration parameters f - complete Colebrook-White equation 1 k s 3.09ν = 2.03log + f 12.27H 4q f λ function of relative depth λ ( ) = λ mc Dr

12 Secondary flow model Γ = khρ gs o straight C uv = f ( σ, Dr ) Secondary flow term straight transitional fully meandering Key: C uv Γ total Relative depth Sinuosity

13 Typical distributions f λ Γ C uv Colebrook-White λ = f (λ mc, D r ) Γ fp (-ve) Γ mc (+ve) Γ fp (-ve) Varies with σ, D r Top of bank

14 CES Outputs Cross-section: total flow Q area A conveyance K ave velocity U Re number Fr number α, β Across section: unit flow q unit conveyance k depth-ave U d bed shear stress τ shear velocity U * Fr number f,n l with depth

15 FCF Straight: Large Scale Bed level (m) Depth = 0.249m Lateral distance across channel (m) Bed shear stress (N/m 2 ) Lateral distance across channel (m) Depth-averaged velocity (m/s) Lateral distance cross channel (m)

16 River Blackwater Model Sinuosity = Bed level (m) Lateral distance across channel (m) Depth-averaged velocity (m/s) Lateral distance across channel (m)

17 River Severn, Shrewsbury 1.2 Sinuosity = Depth-averaged velocity (m/s) Elevation (m) Lateral distance across channel (m)

18 Comparison to isis method 0.16 isis 0.14 CES prediction data Stage (m) Glasgow Flume Discharge (m 3 /s)

19 Comparison to isis method River 7.8 Severn at Montford Bridge isis CES Prediction 7.2 data Stage (m) Discharge (m 3 /s) Bed level (m) Lateral distance across channel (m)

20 CES stage-discharge River 2 Main CES central estimate Measured data Credible upper / lower bands Stage m Bed elevation (m) Lateral distance across channel - offset (m) Discharge m 3 /s

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