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Review

Pitch Control of Three Bladed Large Wind Energy Converters—A Review

Fraunhofer Institute for Wind Energy Systems, Am Seedeich 45, 27572 Bremerhaven, Germany
Energies 2021, 14(23), 8083; https://doi.org/10.3390/en14238083
Submission received: 20 September 2021 / Revised: 4 November 2021 / Accepted: 10 November 2021 / Published: 2 December 2021
(This article belongs to the Special Issue Innovative Methods for the Control of Very Large Wind Turbines)

Abstract

:
Modern multi-megawatt wind turbines are currently designed as pitch-regulated machines, i.e., machines that use the rotation of the blades (pitching) in order to adjust the aerodynamic torque, such that the power is maintained constantly throughout a wide range of wind speeds when they exceed the design value (rated wind speed). Thus, pitch control is essential for optimal performance. However, the pitching activity is not for free. It introduces vibrations to the tower and blades and generates fatigue loads. Hence, pitch control requires a compromise between wind turbine performance and safety. In the past two decades, many approaches have been proposed to achieve different objectives and to overcome the problems of a wind energy converter using pitch control. The present work summarizes control strategies for problem of wind turbines, which are solved by using different approaches of pitch control. The emphasis is placed on the bibliographic information, but the merits and demerits of the approaches are also included in the presentation of the topics. Finally, very large wind turbines have to simultaneously satisfy several control objectives. Thus, approaches like collective and individual pitch control, tower and blade damping control, and pitch actuator control must coexist in an integrated control system.

1. Introduction

Large wind turbines are almost exclusively implemented by three-bladed horizontal-axis machines with variable speed and variable pitch. Such machines normally have four operation regions, depending on the wind speed (see Figure 1). In the first region, the machine does not generate power because the wind speed is below the cut-in value. The second region is defined between the cut-in and the rated values. The machine enters Region III when the wind speed reaches its rated value and remains inside until the cut-out value is reached. The wind turbine enters Region IV after the cut-out value, which is when it is shut down. The transition between Regions II and III is called II½.
In Region III, the wind turbine works with overrated wind speed, i.e., the value for which the machine was designed for normal operation. Therefore, the control strategy is designed to limit the rotor speed and the power. The strategy is implemented as a regulator with the rated speed as the reference signal (set point). The way to achieve this objective is to change the angle of attack of the wind with respect to the blades, affecting the aerodynamic forces acting on the blades. This effect is obtained by rotating the blades along their longitudinal axis, i.e., the blade pitching axis.
In the case of very large wind turbines, the mentioned strategy has several problems. Due to the large swept area, the wind does not have a homogeneous spatial distribution. Hence, it has impacts of different intensities on the rotor surface, causing an imbalance of forces. On the other hand, large machines have considerable inertia and, therefore, they are slow to react when the wind speed changes rapidly. The immediate consequence is that the control action must be fast, which also implies a sharp breaking when the set point is reached. This leads, on the one hand, to the occurrence of important loads and, on the other hand, introduces rapid disturbances in the thrust force, which results in vibrations in the blades and tower. Despite the effort to build the blades and other components as similar as possible, it is inevitable that there are differences between them and, as a consequence, mass imbalances are common, which also induce loads.
Finally, the control problem in the full load region is undertaken by pitch control, which in turn has to consider simultaneously regulation of rotational speed and power, rapid response in front of turbulence, damping of vibrations, and reduction of loads. The present contribution is a review of the methods proposed in the literature to address the different problems that have been mentioned previously. Thus, the second section deals with the subject of control, whose objective is the regulation of rotational speed and the different limitations and improvements. In Section 3, the problem of vibration attenuation is described, while the aspects related to load reduction are presented in Section 4. Anti-windup techniques for wind turbine control are summarized in Section 5, and some rules for the tuning of controller parameters are briefly described in Section 6. Section 7 is devoted to the low-level control of pitch actuators. Finally, conclusions are drawn in Section 8.

2. Pitch Control for Speed and Power Regulation

In variable-speed, variable-pitch machines, the rotational speed and the grid frequency are decoupled due to an indirect connection between generator and grid, which is carried out, nowadays, by the so-called back-to-back converters. This concept is about 25 years old (see [1,2,3,4,5,6]). The focus of interest in the current work is limited to pitch control.

2.1. Collective Pitch Control

Collective pitch control (CPC) is probably the oldest and most common control mechanism used to obtain smooth, regulated, and maximized energy extraction in the case of pitch variable machines. It is based on one controller, where the controlled variable is the rotational speed and the control variable is the pitch angle, which is often called the pitch command. This pitch angle is supplied to all three pitch actuators equally. Figure 2 shows the control system configuration for collective pitch control.
Figure 2 also includes the torque control loop only for the sake of completeness. β0 is the value of the pitch angle that defines the operating point. Thus, this is the pitch angle necessary to maintain the generator speed at the rated value when the linear controller delivers a control signal equal to zero, because the controlled output has reached the set point.

2.2. Control Laws Applied to the CPC

The control system configuration is practically standard. However, the control laws used to implement the CPC can be different. The classic approach is based on PI control.

2.2.1. Standard PI/PID Controllers

A common control law applied to wind turbines is the PI/PID (proportional, integral, derivative). Thus, PID controllers have been studied and used in industry [7,8,9] as well as in academia (e.g., see [10,11,12]). The application of PID control to wind energy systems dates back to the 1970s and 1980s, as is reported, for example, in [13,14].
There are several configurations for a PID controller. The most common form used in the field of wind energy control is the parallel form [12] given by the transfer function
G PID ( s ) = K p + K i s + K d s 1 + T d s .
Kp, Ki, and Kd are the coefficients that have to be tuned in order to obtain optimal behavior. The 1/Td is the cut-off frequency for a low-pass filter that limits the high frequencies of the derivatives part. The first order low-pass filter in the derivative part is necessary for practical implementation, since a pure derivative term is a noncausal system.

2.2.2. Nonlinear PI/PID Controllers

Large-sized wind energy converters are characterized by flexible structures, nonlinearities in the pitch actuators as well as in the aerodynamics, and many operation points. Thus, standard control laws become unsatisfactory for maintaining an acceptable level of control performance. An alternative is to implement a PI/PID control system, where the controller parameters are adjusted by using nonlinear functions of the control error. This procedure is normally called NPI/NPID (Nonlinear PI/PID, see, e.g., [15,16,17]).
The control law is defined by the following:
G NPID ( s ) = f p ( e ) + f i ( e ) s + f d ( e ) s ( 1 + T d s )
where functions fj(e), with j = p, i, and d, are given, for instance, by the following nonlinear function:
f j ( e ) = K 0 j + K 1 j [ 1 sech ( K 2 j ( e ) ]
Hence, the controller gain is given by K0 + K1, in the case of large control errors, and by K0 for small errors. K2 defines the shape of the adapting curve.
NPID approaches have successfully been used in robotics. Its use for the control of wind turbines can be found in [18,19].

2.2.3. Fractional Order PI/PID Controllers

The fractional order PID (FOPID) control, which is also known as PIνDμ with ν and μ as fractional orders, is proposed in [20]. It has been remarked in [21] that the FOPID enhances the performance of the PID control, since the fractional orders contribute two additional parameters, augmenting the possibility of tuning. Furthermore, it is more insensitive to parameter uncertainties.
FOPID control has aroused interest in academia and industry (e.g., see [22,23,24]). The anti-windup problem of FOPID is studied in [25]. The need to use gain-scheduling adaption together with FOPID is presented in [26], where the FOPID includes an anti-windup mechanism for actuators with limited magnitude is applied to a hydroelectric power station. The FOPID controller is short-formulated here, according to [27]. Starting from (1), the FOPID is obtained as a generalization by introducing fractional exponents ν and μ to the Laplace variable s; i.e.,
G FOPID ( s ) = K p + K i ( 1 / s ν ) + K d ( 1 / s μ ) + T d ,
where (1/sγ) is an integrator with γ real and positive. A continuous integro-differential operator can be expressed as follows:
X ( s ) = K s γ , γ .
The exponent γ in (5) is negative in the control law (4). For the implementation of (5), several approximations are available (see [28,29,30]). The application of a FOPID to the collective pitch control of a large wind turbine is presented in [31].

2.2.4. Fractional Order Nonlinear PI/PID Controllers

The NPID can be combined with the FOPID in order to obtain a fractional order nonlinear PID (or PI) control (FONPID or FONPI). The control law is formulated as follows:
G FONPID ( s ) = f p + f i ( 1 / s ν ) + f d ( 1 / s μ ) + T d ,
where the functions (f) as well as the orders, ν and μ, are defined in the previous subsections. This approach is used for the pitch control of wind turbines in [32].

2.2.5. Collective Pitch Fuzzy Control

Fuzzy control [33,34,35] is a formulation of control systems which is based on fuzzy mathematics (i.e., fuzzy sets, fuzzy logic, and fuzzy systems; see, for instance, [36,37,38]). The advantage of the approach is the possibility to introduce inaccurately and linguistically described information into a control system, whose formulation is mathematically formal. A typical fuzzy controller consists of four main components: a fuzzification interface, the inference machine, the rule base, and the defuzzification interface (see Figure 3).
The collective pitch control of a wind turbine has been implemented by using a fuzzy controller many times. Some of these works are, for instance, [39,40,41,42]. In [43], the CPC combines a PID controller and a fuzzy controller. The final control law includes a fusion factor (κ), such that
u ( t ) = κ u P I D ( t ) + ( 1 κ ) u F u z z y ( t ) .
When the control error is small, a large value of κ is chosen such that the focus is put on the PID in order to compensate for the steady state error. When the control error is large, κ is small, centering the attention on the fuzzy control in order to speed up the response. A similar configuration, but including a linear quadratic (LQ) controller instead of a PI, can be found in [44]. However, the last one uses controller switching and not controller fusion.

2.3. Collective Pitch Neural Control

The use of neural networks has proven to be an important tool to approximate multidimensional input–output general functions. Thus, one application field of neural networks is control system design [45,46], in particular for nonlinear systems. Therefore, it is also attractive for the implementation of pitch control of wind turbines. An important drawback of neural networks is the fact that they are not dynamic, i.e., they can only be used for the representation of static functions. Thus, the time dependence that characterizes a dynamic system has to be provided outside the neural network.
There are several architectures available for the implementation of a neural network. Radial basis function networks (RBF) [47] seem to be preferred for the implementation of control systems because they include only one hidden layer, a linear output node and a simple learning algorithm. However, multi-layer perceptrons (MLP) and deep neural networks (DNN) [48] are also applied.
The application of neural networks to the pitch control of wind turbines is distinguished by two main concepts: the direct control, i.e., the neural network is the controller, and the hybrid approach, where a classic controller, like PI or PID, is combined with the neural network, whose function is to adjust the controller parameters to the operating point in a similar way as the gain-scheduling mechanism does.
The application of neural control to pitch control of wind turbines is varied and multifaceted. Only a few relevant works are considered as examples in the following. In the case of RBF networks, it is more common to find hybrid approaches. For example, an RBF/PI configuration can be found in [49], an RBF/PID in [50], and an RBF/FOPID in [51]. The latter is a complex approach with the objective of achieving load mitigation. For the training, a set of controller gains and orders for each wind speed is used. Simulation results show some improvements. However, the approach uses a collective pitch control configuration, and, therefore, the load reduction is limited. RBF direct control approaches are also reported in the literature, as, for example, [52,53]. The last one proposed an adaptive control approach to improve the control performance. On the other hand, the pitch angles resulted in being larger.
MLP networks are used as direct controllers in [54,55]. The controller of [54] performs satisfactorily if the wind speed does not change very fast. In such a case, the pitch angles present some slow frequency oscillations. In [55], a comparison with an RBF controller is included as well. Both controllers work satisfactorily, though the RBF approach outperforms the other slightly.
Back propagation (BP) is another network architecture that can be found in the literature for both direct control [56] and hybrid control [57]. In [57], a PI controller with gain-scheduling is compared with a PI controller with a back propagation (BP) neural network. Performance results are similar with a slightly superior behavior for the BP approach.
Finally, studies based on deep neural networks have been reported recently. They can be found, for e.g., in [40,58]. Both approaches use a deep learning mechanism for wind speed estimation. This is combined in [40] with a fuzzy pitch controller and, in the second work, with a hybrid RBF/PI controller. Neural controllers based on deep neural networks are not common.

2.4. Adaption

Wind turbines are characterized by nonlinear dynamics. Hence, in order to use a linear controller, an operating point (u0, y0) must be defined, and the control system has to be set to work on it, as is shown in Figure 4. The problem with wind turbines is the fact that the operating point is not static, but changes with the wind speed, which is a stochastic variable. If the controller is optimally tuned to operate at a defined wind speed, it will experience degraded performance when the wind speed changes. Therefore, an adaptive control law is necessary (e.g., see [59,60,61] for adaptive control).
The simplest scheme of an adaptive control system is the gain-scheduling approach. The basic idea corresponds to determining a family of operating points and for each operating point to tuning the corresponding controller. Then, an operating point detector is used to set the correct controller parameters. Thus, there are different mechanisms for parameter adaption and for the detector.
In the case of wind turbine pitch control, it is very common to tune the controller parameters for each wind speed between the rated value and the cut-out with a desired resolution, to organize the parameters in a look-up table, and to use an anemometric measurement of the wind speed to select the parameters from the look-up table. Another approach is implemented by using several controllers placed in parallel, but only one is connected to the output. Controllers are switched on according to a variable that selects the controller depending on the operating point [62]. In order to obtain a bumpless switch, the conditioning technique can be used [63]. The switching variable is a measurement or estimation of the wind speed.
Alternatively, a unique parameter sensible to the operating point changes (the scheduling parameter) is defined and the controller parameters are derived as a function of this parameter. Thus, the controller is continuously adjusted according to the variation of the scheduling parameter. In the field of wind turbine control, this is the approach used, for instance, in [64,65,66]. It is derived on the basis of a second order model of the drivetrain by using a PI controller and the pole placement approach. The scheduling parameter is the sensibility function ∂P/∂β or ∂Ta/∂β.
A more advanced approach assumes the wind turbine as a linear parameter-varying (LPV) system and the control system includes a gain-scheduling approach [67,68]. Another alternative is to use a neural network, as described in the previous subsection.

2.5. Collective Pitch Control with Maximum Power Limitation

Sometimes, power fluctuations can be important. Therefore, a protective control loop is added in [69,70]. The idea is illustrated in Figure 5, where two control loops can be observed. The former is the standard collective pitch control, and the latter is a power limiter, where the set point is the maximum design limit for the power. As a control law, PI control is often used.

2.6. Improvement by Using Feed-Forward Control

If a measurement or an estimation of the effective wind speed is available, the performance of the collective pitch control can be improved by using a feedforward approach. The control system configuration is shown in Figure 6, where v ^ w e is the estimation of effective wind speed or a measured value of the wind speed, which has been transferred and scaled to the center of the hub.
The approach uses the measured or estimated disturbance to produce an anticipative control signal that is injected together with standard control action, such that the wind turbine reacts at the moment that the disturbance reaches the system [71]. In order to obtain the desired effect, the feedforward control must reach the same point in the system with the same magnitude but the opposite sign.
Feedforward control is relatively new in the field of wind turbines and both approaches, using measurements and estimations, are present in the literature. LiDAR measurements (light detection and ranging) are used, for instance, in [72,73]. Feedforward based on wind speed estimation is reported in [74,75,76]. The feedforward control is normally combined with the collective pitch control. However, the feedforward control is also combined in [77] with a CPC in a control configuration that also includes an IPC control.

2.7. Estimation of the Effectve Wind Speed

As previously described, the feedforward control requires an estimation of the wind speed. A large wind turbine has a rotor that sweeps across an extensive area. Hence, the wind speed is not uniformly distributed and also not homogeneous; therefore, a single point speed measurement, like that obtained from a nacelle anemometer, is not useful for control purposes. On the other hand, the forces caused by the wind acting on the rotor blades are transferred to the rotating shaft. The shaft integrates the forces into a torque that drives the wind turbine.
It is advantageous to find a fictitious wind speed point acting on the center of the hub, which is applied to a dynamic model of the wind turbine to produce the same power output and rotational speed as the real wind turbine under a real wind field [78]. However, the effective wind speed is not measurable and, hence, several approaches are available for its estimation.
A broad review of approaches for effective wind speed estimation is available in [79]. The most common are based on observer [80] or Kalman filters [81]—observer for an unknown input [82], immersion, and invariance estimator [83]. Other methods, such as power balance estimator [78], disturbance–adaptive control [84], and data fusion in the frequency domain [85], can also be considered. Finally, the wind speed has also been estimated by using neural networks, as is reported, for example, in [86,87,88].

2.8. Advantage and Disadvantage of the Controllers

In order to implement a collective pitch control system, any known SISO (single input–single output) control laws can be used (see, e.g., [89]). From a practical point of view, all controllers have similar performance, and the choice depends in some way on the preference, background, and expertise of the control system designer. However, there are a few aspects that can also be considered for the selection.
The wind turbine is a nonlinear system and the operating point changes with the wind speed, and, therefore, controller adaption is necessary. Classic adaptive control methods, such as self-tuning or model-reference control [59,60,61,90], appear to be too complex for the requirements, and practical experience shows that simple gain-scheduling approaches perform satisfactorily.
PI/PID control is widely used in industry and presents the additional advantage that the gain-scheduling adaption is not difficult to implement. Therefore, PID control has some favoritism in practice. The performance of the PID control can easily be improved by the NPID approach, which also includes a kind of adaption, and also by the FOPID and the FONPID. However, the improved performance takes place at the expense of a higher number of parameters; therefore, the parameter tunning is much more complex. In order to reduce the number of parameters to be tuned, the nonlinear law can be applied only to the proportional gain and the fractional order only to the integrator. Thus, the number of additional parameters is only three. Multi-objective optimization can be used (and is sometimes used) for the tuning of many parameters, but the procedure is not straightforward. In such a direction, more research effort is still necessary.
Finally, fuzzy, as well as neural, controls are also used in academia, but their small performance increase does not justify the complex implementation and tuning. However, a useful application is when the approaches are often combined with PI controls in order to implement parameter adaption, similar to the gain-scheduling mechanism. Deep neural control may be an interesting solution for future very large wind turbines, where retards, due to large inertias and high nonlinearities (due to very flexible components), render conventional control approaches ineffective.

3. Control for Compensation of the Pitching Activity

The growing need for renewable energy necessitates ever-larger wind turbines, and the stiffness reduction caused by mass limits makes the structures more flexible and, as a result, more vibration prone. Vibrations can be caused by a variety of factors in general, such as, for instance, turbulent aerodynamic loads, adverse environments, and seismically active locations. Constructive aspects like flexible high towers with a large mass at the top can also lead to important oscillations.
Since the first vibrational mode of the tower in the fore-aft direction is very low-damped, tower oscillations will appear due to the blade pitching because the pitching activity disturbs the aerodynamic thrust force [91], which in turn is transferred through the structure to the tower. All these vibrations are transferred to the blades as well [92]. A comprehensive study of wind turbine vibrations can be followed in [93,94,95,96,97,98,99,100]. The control system can also be used to attenuate large oscillations. Hence, pitch control with damping injection to reduce oscillations is analyzed in the following.
The general concept has its origin in the passivity-based energy shaping plus damping injection controller design methodology proposed for robotic manipulation [101,102,103]. The idea is to add artificial damping by superimposing a proportional term including velocity feedback into the control law. A second order model with a damping term proportional to the movement speed is normally used. The procedure can also be applied to increase the damping of the tower and blades.

3.1. Active Tower Damping Control

The control objective is to reduce tower oscillations caused by the pitching activity. This is accomplished by increasing the injection of tower damping, whose implementation is a complementary control loop. It is called active tower damping control (ATDC).
A simple integral control law is proposed in [91], which can be formulated as follows:
Δ β atdc ( s ) = D t ( F t / β ) β 0 1 s X t ( s ) ,
where ∂Ft/∂β is the sensitivity function of the thrust force in terms of the pitch angle at the operating point β0. Figure 7 shows the control system configuration.
Figure 7 also shows the direct coupling between CPC and ATDC. This aspect has also been pointed out in [104]. Moreover, the actions of both controllers are contradictory: the CPC introduces strong pitch activity in the presence of turbulence, which in turn leads to tower oscillations; on the other hand, the ATDC reduces the fluctuations by changing the pitch angle, i.e., acting against the CPC. Therefore, the controller tuning consists of finding a compromise between both control loops. A solution to the tuning problem is proposed in [105], where the methodology is based on a cooperative game-theoretic approach. It solves the problem by using multi-objective parametric optimization and a decision maker. An effective way to solve cooperative games is to use the Pareto methods of multi-objective optimization (MOO), which can be reviewed in [106,107,108,109].
CPC and ATDC can also be combined in the same way but using more advanced control algorithms. For instance, nonlinear PID algorithms are used in [18] and fractional order PID control is studied in [31].

3.2. Active Blade Damping Control

The damping injection technique can also be used for the damping of blade tip vibrations. However, this is not a common finding in the literature. Such an idea is proposed in [110] for a collective damping of edgewise vibrations, since the edgewise mode is poorly damped with respect to the flapwise mode [111]. The control law is expressed, in terms of the tip deflection, by
Δ β abcd ( t ) = D db R [ ω b ω r ] ,
where Ddb is the controller coefficient, R is the rotor radius, ωr is the rotor speed, and ωb is the speed of the blade tips. Since the difference (ωbωr) is not measurable, an estimation is needed. The estimation requires a model that includes this difference, such as those studied in [112].

4. Pitch Control for Load Reduction

4.1. Loads in Wind Turbines

The wind turbine is subjected to forces and moments, i.e., loads, which are transmitted through the aeroelastic couplings, affecting both the components and the machine as a whole. For instance, rotor blades are affected by bending forces that take place in the rotor plane as well as perpendicular to it. Furthermore, there are forces acting on the tower and on the nacelle that cause yaw and tilt moments that, in turn, twist and bend the tower.
Following [113], loads can be divided into five different categories. However, loads that contribute to fatigue damage in turbine structures, decreasing lifetime and increasing maintenance costs, are of special interest.
As a consequence of the periodic rotation, cyclic loads naturally appear in wind turbines. As a result, loads occur at a frequency of one per revolution, i.e., 1P, and the loads are referred to 1P loads. Hence, the symbol 1P represents the main rotational frequency (rotor angular speed), while the symbols 2P, 3P… nP correspond to the higher harmonic components of this rotor angular speed. A Fourier analysis of the forces and moments reveals that unsteady loads are centred on the 1P, 2P, etc., frequency components [114].
In particular, loads affecting the blades are focused on the 1P component with respect to the nonrotating reference frame [115]; however, on the other hand, the drivetrain, the hub and the non-rotating structure are primarily affected in the stationary reference frame by 3kP fatigue load components (with k = 1, 2, L). However, the last statement is only true when the behaviour is assumed to be linear and stationary. Contrarily, 1P components can also be found in fatigue loads affecting the drivetrain, hub, nacelle, tower, and other components [116].
As a result of the 1P loads, axial aerodynamic forces vary in every blade with a phase shift of 120 degrees. They can be observed in the flapwise bending moments and, consequently, in the rotor tilt and yaw moments. The 1P loads are caused in general by gravity, yaw misalignment, spatial turbulence and wind shear.

4.2. Indivitual Pitch Control Based on Transformation

The control objective in the full load region is not only the power limitation provided by the CPC but also the attenuation of the loads mentioned above. In order to accomplish a compromise between these two objectives, the pitch angle provided by the collective pitch control is individually adjusted for each blade. The technique is known as individual pitch control (IPC) and has been developed and improved for more than twenty years. The IPC uses the measurement of the bending moments at the rotor blade roots and the controllers provide corrections for each pitch angle.
Following the current literature, there are two different concepts for the formulation of the individual pitch control system. The former includes a transformation of the three root bending moments into two orthogonal moments and the latter is built without any transformation. Approaches that include a transformation can also be divided into two cases: approaches based on the Coleman transformation and approaches based on the Clarke transformation. In the present section, methods that include both transformations are reviewed.
The first and best investigated IPC dates from the late nineteenth century. It was first proposed in [117] and later studied and improved in [116]. The approach was inspired by the Coleman transformation, which, in turn, was first known as the Park transformation, used in electrical systems. The approach based on the Clarke transformation was developed later in [118]. The IPC can be configured either as a multi-SISO (single input–single output) control system or as a MIMO (multi input–multi output) control system. Both configurations are represented in Figure 8.
MIMO controllers, including the Coleman transformation for IPC, can also be found in the literature. The reason is justified because tilt and yaw moments are not really decoupled. In such cases, a multivariable control scheme can provide a better result. Several approaches have been experimented with. For instance, a linear quadratic regulator (LQR) [119], a linear quadratic Gaussian (LQG) control [116,120], and a robust control system design [77,104] are reported in the literature.

4.3. Indivitual Pitch Control without Transformation

The name individual blade control (IBC) (see [115,121,122]) was coined to refer to a control system that uses a multi-SISO approach that does not include transformations. It is based on three single controllers, assuming that all three moments are decoupled. In [123], the different approaches to the IPC are compared. While MIMO control without transformation is also possible, it has not been implemented so far. The control scheme for the IPC without transformation is illustrated in Figure 9.

4.4. Control Laws Applied to the IPC

The classic IPC with Coleman transformation uses two standard PI controllers as given in (1), but with Kd equal to zero. This configuration is improved in [19] by using NPI control and in [32] by using FONPI control. In [124], the PI controllers of the IPC are combined with a radial basis function neural network such that the PI controllers are better adapted to the nonlinearities. The results show an important improvement in the load reduction.
In the case of IPC with Clarke transformation, the used control law is the proportional resonant (PR) controller proposed in [125] and given by the following:
G PR ( s ) = K p + k = 1 n K k ω c s s 2 + 2 ω c s + ( k ω r ) 2 ,
where Kk are the individual resonant gains and the index k corresponds to the harmonics 1P, 2P, etc.
The individual blade control, as proposed in [122], is a multi-SISO control system, where the individual SISO controllers can be implemented by using any available control law. However, concrete control algorithms are not mentioned in the literature.

4.5. Analysis and Discusion of the Different Control Schemesfor IPC

Different approaches for the IPC have been developed for the same objective, but the concepts are not equivalent. Embedding the Coleman transformation in the control law, a full coupled MIMO controller is obtained, where the diagonal elements of the transfer matrix are proportional resonant transfer functions as given in (10). All the other six elements are also transfer functions. By embedding the Clarke transformation, a symmetric full transfer matrix with resonant transfer functions in all elements is obtained. Thus, both MIMO controllers are different. While the azimuth angle must be measured in the approach with the Coleman transformation, it is not required for the Clarke transformation or the IBC.
On the other hand, the IBC has a simplified diagonal structure, ignoring cross-coupling interactions. On the other hand, the load information of each individual blade is maintained, something that is lost in the case of approaches with transformation; therefore, the IBC is more flexible to select the loads to be reduced. The cost of this flexibility is the additional controller and the impossibility of considering the blade interactions.

5. Anti-Windup Techniques for Pitch Control

5.1. Classic Anti-Windup Techniques

Controllers with integral action require a technique to avoid the windup of the integrator. With respect to PID control, anti-windup mechanisms have been studied in depth for a long time (see, for instance, [126,127,128]). In the following, the problem is considered for a controller, such that it is valid for the whole family of PID control laws. On the other hand, an anti-windup strategy for the FOPID is described in [25].
For the conventional parallel representation of the PID controller, an important strategy is represented by the back-calculation approach, which is proposed in [129] and shown in Figure 10.
The controller can be formulated in the automatic reset configuration, for which a very simple anti-windup strategy is described in [12]. This is also presented in [130] as an external reset. The scheme is presented in Figure 11.
This strategy has the disadvantage that no parameter is available to tune the anti-windup reaction. Therefore, the configuration is modified in [31], as shown in Figure 12, such that a back-calculation strategy is obtained.

5.2. Anti-Windup Techniques for Magnitude and Rate Limitations

The anti-windup mechanisms described above work correctly in the case of actuators with magnitude saturation. However, some actuators, such as, for example, the pitch actuators of wind turbines, are not only limited in magnitude, but also in rate. Hence, an anti-windup mechanism for magnitude and rate limitations is necessary.
It is pointed out in [130] that the external reset scheme appears to change the rate at which the error is integrated, allowing integral action to match the speed of the actuator. This is also correct for the schemes of Figure 13.

5.3. Anti-Windup Technique for Fractional Order Controller

In [25], an anti-windup scheme for FOPID is proposed. The idea is to change the order of the derivative action from μ to σ > 1, when the actuator saturates, such that the derivative action becomes more aggressive, and the control variable leaves the saturation state more abruptly. The concept is illustrated in Figure 14.

5.4. Anti-Windup Technique for the Collective Pitch Control

In the case of the CPC, the problem is given by the fact that there are three nonidentical actuators that can independently saturate only one controller. Although the problem is important, it is seldom treated in the literature. The approach presented here follows [31]. The idea is to fuse the three different signals, ∆βi, into one and to lead the results to the anti-windup scheme. The average value of the following:
β = ( 1 / 3 ) ( β 1 + β 2 + β 3 )
of the three variables can be applied if the three actuators are similar. On the other hand, the worst-case strategy can be used when the differences are important. Due to the fact that the pitch angles in full load operation fluctuate between −3 and 25 degrees, the actuators do not saturate in the negative range. Consequently, the differences (∆β) are always negative or zero for all actuators, i.e., ∆βi ≤ 0, ∀i. For the worst-case strategy, the largest negative difference (maximum saturation) is led to the anti-windup mechanism, i.e.,
β cpc = min 1 i 3 ( β a m a x i β i )   with   β a m a x i β i 0 i .
The anti-windup concept for the CPC is given in Figure 15. The anti-windup mechanism used is presented in Figure 13 or Figure 14.

5.5. Anti-Windup Technique for the Individual Pitch Control

In the case of the individual pitch control, the anti-windup mechanism is more complex. Only some approaches have been proposed in [32,131,132]. The problem includes two dimensions: on one hand, controllers and actuators are separated by the inverse Coleman transformation and, on the other hand, there are two controllers and three actuators. Moreover, the actuators share the IPC and the CPC. Thus, the anti-windup strategy should include not only the IPC but also the CPC.
The solution presented here follows [32]. The solution considers first a virtual actuator, i.e., an actuator with an input only for the IPC control variable βipc,i, or in other words, an actuator with an output reduced by the factor (β0 + βcpc), i.e.,
β i p c i = β a i β c p c β 0   with   i = 1 , 2 , 3 .
The differences in ∆βipc,i are computed in the non-rotating frame and the controllers are in the rotating frame. As a result, the differences must be transferred to the rotating coordinating system by means of a direct Coleman transformation. Since the Coleman transformation does not preserve the sign, the anti-windup mechanisms must become active when ∆βi < 0 for any i, where the outputs of the Coleman transformation (noted ∆βd and ∆βq) should also be negative. This is obtained by using the following:
β d = | β a |   and   β q = | β b |   if   any   β i   <   0
The strategy is illustrated in Figure 16.

6. Parameter Tuning for the Pitch Control with Multi-SISO Controllers

As it was shown in the previous sections, the whole pitch control system consists of several control loops and many controllers, which are in general coupled. Hence, it is desired to tune all controllers considering the interactions and contradictory objectives. An approach for obtaining this is proposed in [133]. It is based on the consideration that all control loops are players in a cooperative differential game [134,135,136], whose solution is provided by a multi-objective optimization problem.
Multi-objective optimization, which is also known as multi-performance, multi-criteria, or vector optimization, was introduced by [137] and many algorithms can be used. Some of them are the NBI (normal boundary intersection [138]), NSGA II (non-dominated sorting genetic algorithm [139]), MOPSO (multi-objective particle swarm optimization [140]), SPEA 2 (strength pareto evolutionary algorithm [141]), NBIm (modified NBI [142]), DSD (directed search domain [143]), MOACO (multi-objective artificial ant colony optimization [144]), MOABC (multi-objective artificial bee colony algorithm [145]), MOBA (multi-objective bat algorithm [146]), DSD II (second version of DSD [143]), NSGA-III (third generation of NSGA, [147]), MOGWO (multi-objective grey wolf optimization [148]), MOM-VO (multi-objective multi-verse optimization [149]), and MOALO (multi-objective ant lion optimization [150]).
The application of this method, based on parametric multi-objective optimization to pitch control, has been reported in [105,110,151,152,153].

7. Low-Level Control of Pitch Actuators

Pitch actuators are modelled by using different levels of complexity. For instance, the pitch subsystem is represented by a first order system in [154,155,156]. Pitch actuators are normally represented by a simple linear model. However, real pitch actuator components have an embedded additional controller.

7.1. Models of Pitch Actuators without Control

In particular, an electromechanical actuator is modelled as a first order system in [157], according to the following:
β ˙ ( t ) = ( 1 / τ ) [ β ref β ( t ) ] ,
where β is the pitch angle and βref is the set point defined as a pitch angle. The pitch angle and the pitch rate are also constrained by the following:
β ˙ m i n β ˙ β ˙ m a x   and   β min β β m a x .
It should be remarked that the maximum amplitude constraint, βmax, for the pitch angle, when the wind speed is overrated, is defined as the necessary pitch angle to maintain a rated rotor speed at the maximum permitted wind speed. On the other hand, βmax is set at 90° during the shutdown operation. A graphical representation of the model is presented in Figure 17.
Some pitch actuators work with a pitch rate set point, i.e., β ˙ r e f . In such a situation, the block diagram of Figure 17 has to be modified to accept pitch rate set points. This change is illustrated in Figure 18.
Second order linear models are used to describe pitch actuators (see, e.g., [158,159,160,161]). Moreover, the second order models can be complemented, as in [162,163], by a dead time Tt. A general second order approach can be described by
β ¨ = 2 ζ ω n 2 β ˙ + ω n 2 [ β r e f ( t T t ) β ] ,
with the same constraints as for the first order model, i.e.,
β ˙ m i n β ˙ β ˙ m a x   and   β m i n β β m a x
The corresponding block diagram is given in Figure 19.

7.2. Models of Pitch Actuators with Control

Pitch actuators normally have an embedded controller. Assuming a PI controller in the pitch actuator control system. The block diagrams change as given in Figure 20 for the first order actuator and in Figure 21 for the second order actuator.

7.3. Pitch Actuators with Fault-Tolerant Control

Fault-tolerant control (e.g., see [164,165]) is a concept whose origin goes back to the birth of safe critical systems, which are not allowed to fail, e.g., an aircraft. Nowadays, the idea has been extended to other kinds of systems, including wind turbines (see [166] for review). The main idea is to define an alternative mission for the system with a finite completion time. This mission has to be fulfilled by the system in the case that a fault occurs. The execution of the mission allows, on one hand, to avoid the crash and, on the other hand, to organize maintenance arrangements and to plan the shutdown, in order to reduce the downtime.
The performance improvement of the pitch control system normally requires major pitching activity leading to increased wear of the pitch actuators. Since actuators and sensors of wind turbines are also prone to faults [167,168], it is expected that pitch actuators will become a weak point in normal operation. For this reason, several concepts for fault tolerant control (FTC) for pitch actuators have been studied.
Pitch actuators are divided into hydraulic and electric systems. The wind energy large converter market has been dominated by hydraulic pitch actuation. They are compact, have a rapid response, and have a high pitching torque. The main disadvantages are the nonlinear behaviour and the hybrid nature (hydraulic power source with electrical control and sensing). The pitch actuator has bias error because of oil leakage in the hydraulic piston, as well as the pitch actuator getting stuck, caused by valve blockage in the hydraulic actuation system, are the most common faults. They are also the most intensely treated cases of fault-tolerant control of pitch actuators (see, for instance, [169,170]).
On the other hand, electric actuators have progressively been adopted because of their simple drive architecture, high reliability, and a unified electric system for power source, sensing, and control. They also have large inertia and the intensive pitching activity can cause overheating and damage. A fault-tolerant control approach for an electrical pitch actuator has been proposed in [171]. However, this field should be studied more exhaustively.

8. Conclusions

The pitch control system is essential, not only for high energy conversion, but also to guarantee a long lifetime of very large wind turbines. In the past twenty years, many control objectives, approaches, and particular techniques have been proposed in order to solve the control problems with which wind energy technology has challenged control engineering. The present review intends to put into context the multifaceted aspects related to the pitch control of wind energy converters and highlight different solutions contributed by the research community.
Performance improvement, prolongation of lifetime, and reduction of vibrations are the main facets of wind turbines. These three aspects are analyzed separately in the work, showing the available approaches for each case. In general, different control schemes for the same control objective perform similarly. Thus, the choice depends on control system designers, where their background, experience, and preferences play an important role.
Control laws more complex than PI/PID normally improve control performance. For instance, FONPI control improves the performance of IPC. However, the implementation and tuning require additional effort that sometimes is not justified in the analysis of the final balance. Moreover, anti-windup mechanisms are essential for all controllers that include integral action. Intelligent control techniques are seldom applied in practice. However, standard techniques will provide limited performance in the case of very large flexible wind turbines. In such a case, intelligent control might become important as a possible solution. Fault-tolerant control of pitch actuators is practically not considered at present, but it is an important concept to increase the reliability of large machines.
Another factor to consider is the fact that very large wind turbines need control for all the objectives presented. Hence, CPC, IPC, ATDC, and ABDC should be included in the integrated control system. A summary of the control objective and approaches are presented in Table 1.

Funding

This work has been financed by the Federal Ministry of Economic Affairs and Energy (BMWi).

Conflicts of Interest

The author declares no conflict of interest.

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Figure 1. Operation regions of a variable-speed, variable-pitch, horizontal-axis wind turbine.
Figure 1. Operation regions of a variable-speed, variable-pitch, horizontal-axis wind turbine.
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Figure 2. Collective pitch control system, including the torque control loop.
Figure 2. Collective pitch control system, including the torque control loop.
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Figure 3. Control system based on a fuzzy controller.
Figure 3. Control system based on a fuzzy controller.
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Figure 4. Control system configuration for a nonlinear system with a linear controller.
Figure 4. Control system configuration for a nonlinear system with a linear controller.
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Figure 5. Power delimiter control as additional control loop for the collective pitch control system.
Figure 5. Power delimiter control as additional control loop for the collective pitch control system.
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Figure 6. Power delimiter control as additional control loop for the collective pitch control system.
Figure 6. Power delimiter control as additional control loop for the collective pitch control system.
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Figure 7. Control system configuration including an active tower damping control loop.
Figure 7. Control system configuration including an active tower damping control loop.
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Figure 8. General configuration of an individual pitch control system with transformations.
Figure 8. General configuration of an individual pitch control system with transformations.
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Figure 9. Control system configuration of the IPC without transformation.
Figure 9. Control system configuration of the IPC without transformation.
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Figure 10. Fractional order nonlinear PID controller with back-calculation anti-windup approach.
Figure 10. Fractional order nonlinear PID controller with back-calculation anti-windup approach.
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Figure 11. Automatic reset configuration with separated integrators and anti-windup strategy.
Figure 11. Automatic reset configuration with separated integrators and anti-windup strategy.
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Figure 12. Back calculation technique embedded in the automatic reset configuration.
Figure 12. Back calculation technique embedded in the automatic reset configuration.
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Figure 13. Modified automatic reset configuration for magnitude and rate with back calculation.
Figure 13. Modified automatic reset configuration for magnitude and rate with back calculation.
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Figure 14. Anti-windup concept taking advantage of the fractional order approach.
Figure 14. Anti-windup concept taking advantage of the fractional order approach.
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Figure 15. Anti-windup strategy for the collective pitch control.
Figure 15. Anti-windup strategy for the collective pitch control.
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Figure 16. Anti-windup strategy for the whole pitch control system (CPC and IPC).
Figure 16. Anti-windup strategy for the whole pitch control system (CPC and IPC).
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Figure 17. Model representation of a first order pitch actuator without controller and pitch angle set point.
Figure 17. Model representation of a first order pitch actuator without controller and pitch angle set point.
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Figure 18. First order model of the pitch actuator with pitch rate set point.
Figure 18. First order model of the pitch actuator with pitch rate set point.
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Figure 19. Pitch actuator model based on a second order system with dead time.
Figure 19. Pitch actuator model based on a second order system with dead time.
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Figure 20. First order pitch actuator with PI control and pitch rate set point.
Figure 20. First order pitch actuator with PI control and pitch rate set point.
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Figure 21. Second order pitch actuator with PI control and pitch rate set point.
Figure 21. Second order pitch actuator with PI control and pitch rate set point.
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Table 1. Summary of methods used for the pitch control of large wind turbines.
Table 1. Summary of methods used for the pitch control of large wind turbines.
Control ObjectiveApproachCharacteristics
Power regulationCollective pitch control (CPC)Power and speed regulation. Several algorithms are available. Standard: PI/PID. Variations: NPID, FONPID. Others: Fuzzy control, neural control, hybrid schemes.
Control with maximum power limitationIt is an additional control loop for a maximum hard power limitation and normally uses a PI controller.
Collective pitch control with feedforward compensationIt requires an estimation of the effective wind speed. The feedforward schme increases the performance of the CPC.
Compensation of the pitching activityActive tower damping control (ATDC)It requires the integration of fore-aft tower-top acceleration. It reduces tower oscillations.
Active blade damping control (ABDC)It requires the estimation of the blade tip deflection speed and reduces blade oscillations.
Control for load reductionColeman-based Individual Pitch Control (IPC)It requires the measurement or estimation of the azimuth angle. It uses the Coleman transformation.
Clarke-based IPCIt uses the Clarke transformation and a proportional resonant controller. Performance is similar to IPC. The azimuth angle is not necessary.
Individual Blade Control (IBC)It uses three independent controllers, ignores coupled effects, considers individual blade loads.
Control of pitch actuatorsStandard actuator It normally uses an internal PI control.
Actuator with fault-tolerant control (FTC)FTC is oriented to hydraulic actuators. Electrical actuators are becoming more common. Hence, FTC should be studied.
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Gambier, A. Pitch Control of Three Bladed Large Wind Energy Converters—A Review. Energies 2021, 14, 8083. https://doi.org/10.3390/en14238083

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Gambier, Adrian. 2021. "Pitch Control of Three Bladed Large Wind Energy Converters—A Review" Energies 14, no. 23: 8083. https://doi.org/10.3390/en14238083

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Gambier, A. (2021). Pitch Control of Three Bladed Large Wind Energy Converters—A Review. Energies, 14(23), 8083. https://doi.org/10.3390/en14238083

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