Exploring the limits in Individual Pitch Control S. Kanev and T. van Engelen - PowerPoint PPT Presentation

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Exploring the limits in Individual Pitch Control S. Kanev and T. van Engelen

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S. Kanev and T. van Engelen Overview Blade load reduction by individual pitch control (IPC) Rotor balancing by IPC Gain-scheduling Dealing with actuator constraints ... – PowerPoint PPT presentation

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Title: Exploring the limits in Individual Pitch Control S. Kanev and T. van Engelen


1
Exploring the limits in Individual Pitch
ControlS. Kanev and T. van Engelen
2
Overview
  • Blade load reduction by individual pitch control
    (IPC)
  • Rotor balancing by IPC
  • Gain-scheduling
  • Dealing with actuator constraints (anti-windup)
  • Simulation results

3
IPC for blade load reduction
  • Pitch control algorithms
  • collective pitch control for keeping rotor speed
    at rated
  • individual pitch control for load reduction
  • Blade load reduction usually flapping moments Mz
    are reduced around the 1p frequency, achieved by
    cyclic pitching.
  • Aerodynamic/mass unbalance results in a static
    shaft load, can be counteracted by offsets on the
    blade pitch angles.
  • Starting point for IPC design LPV model
  • Working point

4
Coleman transform
  • For fixed p, above model is azimuth dependent gt
    LTV model
  • Coleman transformation makes the model LTI
    simplifying controller design.

non-rotating coordinates
rotating coordinates
5
Basic IPC design
  • After Coleman transformation, model gets LTI for
    a given working point
  • 1p blade flap-wise loads (Mz) become static 0p
    rotor moments Mcm !
  • Hence, integral action should be included in the
    IPC controller.
  • Tilt and yaw channels are almost decoupled at low
    frequencies, gt SISO approach
  • FIPC includes series of band-stop filters around
    the 3p and 6p frequencies. Gains computed to
    achieve desired gain margin (e.g. 2)
  • To cover the whole working range, gain scheduling
    should be applied.

6
IPC controller implementation
  • Once the IPC is designed, the transformation
    matrices are added to the controller

7
Rotor balancing by IPC
  • Imperfections in the blades lead to aerodynamic
    and mass unbalance.
  • Unbalance results in static (0p) loading on the
    shaft, and 1p loading on the tilt and yaw moments
    at the yaw bearing.

Aerodynamic unbalance can be represented by
additional slowly varying terms to the flapping
blade moments
  • It can be compensated by adding quasi-steady
    offsets to the blade pitch angles.
  • Possible measurements
  • aerodyn. unbalance blade root bending (0p), or
    shaft (0p), or rotor tilt/yaw moments (1p)
  • mass unbalance either shaft (0p), or rotor
    tilt/yaw moments (1p)
  • Since with strain gauges 0p measurement is
    problematic, other alternatives are under
    investigation (tower top accelerations at 1p).

8
Rotor balancing IPC scheme
  • Assuming blade root moments measurement, the
    rotor unbalance compensation scheme is similar to
    the IPC scheme for blade load reduction
  • Transformation
  • At low frequencies, transformed system
    approximated as static, LTI, and diagonal.
  • Controller structure

Parameters chosen to get critically damped CL
system with desired settling time (e.g. 50 sec).
9
Dealing with constraints
  • Blade pitch actuators have limits
  • Ensuring these in the control algorithm
    especially important for controllers with
    integral term (such as both CPC and IPC).
    Otherwise windup can occur, which can lead even
    to instability.
  • Actuation freedom is distributed between CPC and
    IPC as follows

actuation freedom for CPC
IPC can use remaining actuation freedom
10
Pitch limits in non-rotating coordinates
  • Total pitch angle reference for i-th blade
  • Actuation freedom remaining for IPC
  • Defining
  • The goal is to express the constraints
  • In terms of constraints on ?cm,2 and ?cm,3 (too
    technical, ref. paper).

IPC term
11
Anti-windup IPC implementation
  • To properly implement the constraints in the IPC
    controller, the integrator state should be driven
    by the constrained signal.

The limiters can be implemented as follows
12
Simulation model
  • Nonlinear simulation model used for validation of
    IPC methods
  • TURBU structural dynamics model (156 states),
    consisting of 14 blade elements, 15 tower
    elements (each with 5 dofs), 6 dofs rotor
    shaft, 12 dofs pitch actuators
  • Detailed aerodynamics module, incl. dynamic
    wake, oblique inflow modeling (Glauert)
  • Basic controller for rotor speed regulation and
    power control
  • IPC control for blade load reduction at 1p and
    rotor balancing, incl. actuator constraints
    (anti-windup implementation)
  • realistic blade effective wind speed signals,
    incl. deterministic (shear, tower shadow, wind
    gusts) and stochastic (turbulence) components.
  • Simulation at mean wind speed of 20 m/s, yaw
    misalignment of 10 degrees.
  • Aerodynamic unbalance modeled as blade pitch
    angle offsets of -1, 3 and -2 deg.

13
Scenario 1 IPC for blade load reduction
  • Case 1 without IPC
  • Case 2 with IPC, no pitch limits
  • Case 3 with IPC, with pitch limits

14
Scenario 2 IPC for rotor balancing
  • Case 4 no rotor balancing IPC
  • Case 5 with rotor balancing

15
Scenario 3 IPC for blade load reduction and
rotor balancing
  • Case 6 IPC for rotor balancing and blade load
    reduction, pitch limits included

16
Conclusions
  • IPC can be used for blade fatigue load reduction
    by mitigating the static tilt/yaw rotor moments,
    resulting in cyclic pitching around the 1p
    frequency
  • IPC can be used for compensation of rotor
    unbalance due to blade mass and aerodynamic
    imperfections. This can be achieved by mitigating
    the 0p shaft loads.
  • For rotor balancing IPC, either offset-free
    shaft/blade root bending moment measurements, or
    tower-top tilt/yaw moments measurements.
  • Gain scheduling is needed to cover the whole
    operating region of the turbine
  • IPC action significantly increases the pitch
    speeds and accelerations, requiring to properly
    deal with actuator constraints. The challenge
    here is to transform the original constraints
    into non-rotating coordinates.
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