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Towards robust control design for active flow control on wind turbine blades first results based on numerical simulations Dimitri Peaucelle Caroline Braud, Emmanuel Guilmineau Active flow control on wind turbine blades session - 29 August - 12


  1. Towards robust control design for active flow control on wind turbine blades first results based on numerical simulations Dimitri Peaucelle Caroline Braud, Emmanuel Guilmineau Active flow control on wind turbine blades session - 29 August - 12 :00-12 :25

  2. Objectives ■ Robust control tools for active feedback control of the air flow on turbine blades ● Linear transfer functions representing approximately some dynamics ● Heuristic (or better) design of low order controllers ● Robust analysis of the feedback loop with respect to modeling uncertainties ■ Cooperation with Caroline Braud & Emmanuel Guilmineau ● Choice of a blade profile & actuators/sensors ● Discussion about expected phenomena and objectives ● 1st tests on numerical simulations of the flow ● 2nd tests on a physical benchmark D. Peaucelle 1 SmartEole - Orléans - 29 August 2018

  3. Blade profile & sensors/actuators & numerical measurement D. Peaucelle 2 SmartEole - Orléans - 29 August 2018

  4. Numerical experiments without and with constant air blowing C µ = 0 C µ = 0 . 055 f C µ =0 = 97 . 3408 Hz f C µ =0 . 055 = 102 . 7487 Hz Increased steady-state and amplitude D. Peaucelle 3 SmartEole - Orléans - 29 August 2018

  5. Proposed linear model upstream air flow V 0 k 0 p + + Oscillator wake k p actuation C µ k C µ P p air pressure at point p τ p s +1 at f C µ Hz + + + ˆ k p ˆ τ p s +1 ● Choice of 1st order transfer functions coherent with experiments by Braud&Jaunet ● Model takes into account only dynamics at low frequencies (from 0 to f C µ ≃ 100 Hz) ● Blue part is repeated for each points where air pressure is measured ▲ k C µ and k 0 p identified using steady-state values ▲ τ p identified using phase shift of sinusoids at frequency f C µ ▲ τ p ≃ ˆ τ p assumed similar because almost colocated ▲ k p and ˆ k p identified using amplitude of sinusoids at frequency f C µ ▼ All parameters should be considered as uncertain (modeling and identification errors) ▼ Model at one operating point (eg. one pitch angle α = 0 ) Linear parameter-varying (LPV) could be considered to go further D. Peaucelle 4 SmartEole - Orléans - 29 August 2018

  6. Proposed control problem fluctuation in air flow ∆ V 0 + upstream air flow V 0 k 0 + vector of measured actuation + + C µ Oscillator wake k air pressures k C µ P at f C µ Hz τs +1 + + at several points + 0 . 055 0 ˆ k τs +1 ˆ u control signal W 1 weighted sum of pressures y measurements z performance - + ≃ lift W 2 ( s ) H ǫ error + + band limited filter y c requested value white noise around f Cµ Hz ■ Goal 1 : Make the system asymptotically stable (wake will converge to zero) ● Could be achieved by appropriate feedback control : u ( t ) = H ( y ( t )) ■ Goal 2 : Keep lift at prescribed achievable level ● Control should contain integrator ■ Goal 3 : Attenuate influences of ∆ V 0 and wake on lift ● Can be evaluated by the H ∞ norm of the transfer from ∆ V 0 to z ■ Properties should be robust to modeling, uncertainties, noise & saturation D. Peaucelle 5 SmartEole - Orléans - 29 August 2018

  7. Choice of a simple control structure y = P 131683 + P 168671 ■ y : sum of 2 measures, upstream + close to wake ● upstream : contains mostly information about ∆ V 0 ● downstream : contains mostly information about wake � ∞ ■ PI control u ( t ) = K P ˆ ǫ ( t ) + K I ˆ ǫ ( τ ) dτ + ˆ ǫ ǫ u 0 PI k a - ■ with Anti-Windup ˆ ǫ = ǫ − τ a s + 1( C µ − u ) 0 . 055 0 - + ● Hand-tuned parameters k a τ a s +1 K p = 10 − 2 , K I = − 200 , k a = 10 , τ a = 10 − 5 D. Peaucelle 6 SmartEole - Orléans - 29 August 2018

  8. Open loop simulations with linear model C µ ( t ∈ [0 , 0 . 25]) = 0 C µ ( t ∈ [0 . 25 , 0 . 5]) = 0 . 055 ■ OFF/ON actuator ■ ∆ V 0 periodic positive and negative steps ( 5% variation of V 0 ) P p ( t ) y ( t ) wake D. Peaucelle 7 SmartEole - Orléans - 29 August 2018

  9. Closed loop simulations with linear model y c ( t ∈ [0 , 0 . 25]) = − 1 . 04 y c ( t ∈ [0 . 25 , 0 . 5]) = − 1 . 46 ■ Requested ’lift’ ■ Same ∆ V 0 , noise=0 u ( t ) y ( t ) wake D. Peaucelle 8 SmartEole - Orléans - 29 August 2018

  10. Closed loop simulations with linear model y c ( t ∈ [0 , 0 . 25]) = − 1 . 04 y c ( t ∈ [0 . 25 , 0 . 5]) = − 1 . 46 ■ Requested ’lift’ ■ Same ∆ V 0 , noise � = 0 u ( t ) y ( t ) wake D. Peaucelle 9 SmartEole - Orléans - 29 August 2018

  11. Robustness of closed-loop ■ γ = H ∞ performance of transfert ∆ V 0 → z ● (A) If no uncertainties on parameters ● (B) Constant uncertainties : 10% on τ , 5% on f Cµ , 20% on k C µ ● (C) Time varying uncertainties : 10% on τ , 5% on f Cµ , 20% on k C µ fluctuation in air flow ∆ V 0 + upstream air flow V 0 k 0 + vector of measured actuation + + C µ Oscillator wake k air pressures k C µ P at f C µ Hz τs +1 + + at several points + 0 . 055 0 ˆ k τs +1 ˆ u control signal W 1 weighted sum of pressures y measurements z performance - + ≃ lift W 2 ( s ) H ǫ error + + band limited filter y c requested value white noise around f Cµ Hz γ ( A ) = 0 . 4153 , γ ( B ) ≤ 0 . 4279 , γ ( C ) ≤ 0 . 4563 ● Values computed using R-Romuloc toolbox D. Peaucelle 10 SmartEole - Orléans - 29 August 2018

  12. Conclusions ▲ Simple control strategy based on existing actuators/sensors ▲ Data obtained from numerical experiments ▲ Encouraging simulations and robustness assessments ▼ Need for validation on closed-loop numerical experiments ▼ Need for validation on physical experiments ▼ Physical sensors may not be efficient enough (noise +?) ▼ Actuators may not be efficient enough (saturation + PWM +?) ■ Easily hand-tuned control ● Structured control tools (Hifoo, hinfstruct,...) could do better ■ Current study for one operating point ( α = 0 , one wind speed, etc.) ● Need for parameter-varying control, or adaptive control D. Peaucelle 11 SmartEole - Orléans - 29 August 2018

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