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Blade Element Momentum Theory for Tidal Turbine Simulation with Wave Effects: A Validation Study * H. C. Buckland, I. Masters and J. A. C. Orme

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Presentation on theme: "Blade Element Momentum Theory for Tidal Turbine Simulation with Wave Effects: A Validation Study * H. C. Buckland, I. Masters and J. A. C. Orme"— Presentation transcript:

1 Blade Element Momentum Theory for Tidal Turbine Simulation with Wave Effects: A Validation Study * H. C. Buckland, I. Masters and J. A. C. Orme

2 Introduction Fast and robust turbine computer simulation: Performance, periodic stall Survivability, extreme wave climate Fatigue Fluid flow conditions

3 Outline Turbine Performance simulation BEMT Tidal flow boundary layer Stream function wave theory Wave acceleration Tidal flow + Wave disturbance Validation study

4 Blade element theory dF a1 (a,b) dT 1 (a,b) Inflow profile Waves Tidal stream Numerical aim: dF a1 (a,b) = dF a2 (a,b) dT 1 (a,b) = dT 2 (a,b) Minimise g: g=[ dF a1 (a,b) - dF a2 (a,b) ] 2 + [ dT 1 (a,b) - dT 2 (a,b) ] 2 Momentum theory dF a2 (a,b) dT 2 (a,b)

5 Blade Element Momentum Theory BEMT Momentum Theory

6 Closed System: Unknowns: a, b, T Fa Two pairs of equations: dT_{1}, dFa_{1}, dT_{2}, dFa_{2} Cavitation Blade Element Theory Blade Element Momentum Theory BEMT

7 Optimiser ‘fmincon’ for a closed BEMT system b

8 BEMT steady state example

9 Blade element theory dF a1 (a,b) dT 1 (a,b) Inflow profile Waves Tidal stream Numerical aim: dF a1 (a,b) = dF a2 (a,b) dT 1 (a,b) = dT 2 (a,b) Minimise g: g=[ dF a1 (a,b) - dF a2 (a,b) ] 2 + [ dT 1 (a,b) - dT 2 (a,b) ] 2 Momentum theory dF a2 (a,b) dT 2 (a,b)

10 Tidal boundary layer Bed friction -> boundary layer Permeates the whole water column Power law approximation for boundary layers Assume a constant mean free surface height h x

11 Chaplin’s stream function wave theory C u v Finite depth, 2D irrotational wave of permanent form Frame of reference moves with the wave Finite depth wave theory: Incompressible flow Boundary condition Kinematic free surface condition: Bernoulli equation on the free surface: Mean stream flow Wave Disturbance

12 Tidal flow +wave forces Problems: Depth dependent tide velocity Steady state BEMT Coupling: Doppler effect Alter moving frame of reference

13 Accelerative forces: The Morison equation c Axial oscillatory inflow: Tangential oscillatory inflow:

14 The Barltrop Experiments 350mm turbine diameter 200 rpm 0.3m/s 1m/s Wave height 150mm Long waves 0.5Hz Steep waves 1Hz Bending Moments Mx My Towed to simulate tidal flow! Barltrop, N. Et al. (2006) Wave-Current Interactions in Marine Current Turbines. Tidal turbine in a wave tank 2 seperate investigations

15 Self Weight bending moment

16 Mx My results: 1m/s current

17 The Barltrop Experiments Barltrop, N. Et al. (2007) Investigation into Wave- Current Interactions in Marine Current Turbines. 350mm turbine diameter 200 rpm 0.3m/s 1m/s Wave height 150mm Long waves 0.5Hz Steep waves 1Hz Bending Moments Mx My Barltrop, N. Et al. (2006) Wave-Current Interactions in Marine Current Turbines. 400mm turbine diameter 90rpm 0.7m/s 0.833Hz Varying wave heights 00mm 35mm 84mm 126mm Torque T Axial force Fa Towed to simulate tidal flow! Tidal turbine in a wave tank 2 seperate investigations

18 Axial force and torque

19 TSR vs Ct, Cp and Cfa

20 Conclusion Validation of wave theory Compatibility of dynamic inflow with BEMT Validation of self weight torque Wave effect on performance is dependent on TSR curve profiles

21 Further work Wave superposition Sea spectra, random phase sampling Storm event simulation Two way wave and current coupling


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