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Resilient synergetic control for fault tolerant control system

Radhia Ettouil, Karim Chabir, Dominique Sauter, Mohamed Naceur Abdelkrim

To cite this version:

Radhia Ettouil, Karim Chabir, Dominique Sauter, Mohamed Naceur Abdelkrim. Resilient synergetic

control for fault tolerant control system. 10th IFAC Symposium on Fault Detection, Supervision and

Safety for Technical Processes, SAFEPROCESS 2018, Aug 2018, Varsaw, Poland. �hal-01859252�

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Resilient Synergetic Control for fault tolerant control system

Radhia. Ettouil Karim. Chabir Dominique. Sauter∗∗

Mohamed Naceur. Abdelkrim

University of Gabes, MACS Laboratory, LR16ES22 Tunisia, (e-mail:

radhiaettouil@gmail.com).

∗∗Research Center for Automatic Control of Nancy, Lorraine University, CRAN UMR 7039, BP 70239 Vandeouvre Les Nancy

(e-mail: dominique.sauter@univ-lorraine.fr)

Abstract: In this paper, a resilient synergetic control is established to compensate for parametric actuator faults. The proposed strategy is based on the synergetic approaches to compensate for the dynamics fault effects and maintain the desired performance. The main idea is to estimate fault using an adaptive observer in the first place. Afterwards, the fault estimation will be integrated in the system dynamics. Then, a resilient synergetic control is designed using the new dynamics model. Simulation results prove the effectiveness of the proposed strategy.

Keywords:Synergetic control, adaptive observer, resilient control, fault estimation, pitch system.

1. INTRODUCTION

Wind turbines constitute an interesting part of the re- newable energy production. Reliability, safety and fault tolerant wind turbine control are highly required. To in- crease system reliability, the design of fault tolerant con- trol (FTC) becomes necessary. These systems are control systems that assure tolerating potential faults in the sys- tem in order to improve its reliability and safety while maintaining a desirable performance. In other words, they are closed-loop control systems which compensate for fault and provide a desirable performance. Recently, FTC tech- niques have attracted the attention of several researchers- Gao et al. [2015] and Cecati [2015].

One of the categories of faults is that leading to a large variation in system parameters. As noted in (Noura et al.

[2000]), the occurrence of these faults causes a drastic change in system dynamics and can lead to an abnormal operation of the system. Significant research and numerous strategies have been developed in order to design a spe- cific FTC for that type of faults. A fault reconfiguration approach is proposed in (Steffen [2005]), based on the change of the control structure in response to the fault.

Furthermore, data-driven FTC techniques focus on the problem of the output feedback FTC for a system affected by a fault that changes system dynamics (Kulcs´ar et al.

[2009], Dong [2009], Yin et al. [2014], Ding et al. [2014] and Wang and Yang [2016]). A data-driven output feedback FTC problem considering optimal performance is studied in [15]. Moreover, a projection-based FTC design for pitch systems is presented in (Ding et al. [2012]). Using a new form of extended state observer, a reconfigurable control

Sponsor and financial support acknowledgment goes here. Paper titles should be written in uppercase and lowercase letters, not all uppercase.

based on LPV system modeling is proposed in (Jain et al.

[2013]).

The sliding mode approach is also used for the FTC issue to compensate for the mentioned faults. The sliding mode observer (Edwards et al. [2000]and Patel et al.

[2006]) is used to achieve fault estimation that has been applied to substitute the fault detection and isolation (FDI) approach. Also, a Takagi-Sugeno Sliding Mode Observer (T-S SMO) is proposed in (Jiang et al. [2004]) in order to estimate system actuator parameter faults. A novel FTC allocation schema with output integral sliding mode is proposed in (Hamayun et al. [2013]), when only the system outputs are measured. Recently, an adaptive step by step sliding mode observer has been used in fault tolerant control based on state system estimation and fault indicator (Lan et al. [2016]).

In this work, we present a novel technique for compen- sating for the actuator fault. The new strategy consists in designing a resilient controller using the synergetic theory. The synergetic control allows to drive the system trajectories to operate on the designed manifolds. This ap- proach has been developed by Kolesnikov and Coworkers (Kolesnikov et al. [2000]). The connection and comparison between the synergetic performance and those of sliding mode control have been detailed in Nusawardhana et al.

[2007]. Recently, the synergetic control has been applied in many fields (Ju et al. [2017],Shokouhandeh and Jazaeri [2017] and Bouchama et al. [2016]). The main advantages of this approach are global stability, order reduction and insensitivity to parameter variation. Here, this theory will be used to design a resilient control able to compensate for the dynamic faults and to recover the initial performance.

The remainder of the paper is organized as follows. Section 2 presents the problem formulation. Section 3 introduces

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briefly the synergetic control and the adaptive observer and presents the proposed resilient synergetic control. A numerical example is simulated in section 4. Finally, some conclusions are drawn in section 5.

2. PROBLEM FORMULATION

This work focuses on the low pressure fault that affects pitch system of wind turbines. The faulty system is mod- eled by:

˙

x=Ax+Bu+ ∆Af x

y=Cx (1)

Where, A=

0 1

−ωn2 −2ξnωn

, B=

0

ωn2

, C = [ 0 1 ]

∆A=

0 0

ωf2−ωn2fωf −2ξnωn

wheref denotes the indicator fault,f ∈[ 0 1 ]. ωn andξn

denote respectively the natural frequency and the damping factor, whileωf andξf denote their values at low pressure.

This work aims to design a resilient synergetic control as an FTC technique to recover the desired performance when an actuator fault occurs. Fig.1 shows the general structure of the FTC system:

Fig. 1. General structure of the FTC system

3. DESIGN OF RESILIENT SYNERGETIC CONTROL Our goal is to use the synergetic theory to design a resilient control in order to compensate for the effect of the fault and ensure stability for a closed loop system.

3.1 Synergetic Theory

The design of the synergetic controller is similar to that of the sliding mode controller. The main steps of the procedure can be itemized as follows:

• Design of manifold The manifold s(x) = 0 can be a linear or nonlinear function of the state variables.

It is selected according to the desired performance.

Consider the following dynamical system of a single pitch system in fault-free case:

˙

x=Ax+Bu (2)

The manifold has the form:

M =s(x) = 0 (3)

It is constructed so that det ∂M∂xB 6= 0.

• Design of synergetic control law

The synergetic controller is synthesized by solving the first order differential equation:

TM˙ +M = 0 (4)

with T =TT >0 is a diagonal positive definite ma- trix, presenting the convergence parameter. Solving the above differential equation foruyields a controller that forces the variables state to lie on the manifold s(x). Note that:

dM dt =∂M

∂x

∂x

∂t =

∂xs(x) T

˙

x=sx(x) ˙x (5) Then, solving the above differential equation gives:

TM˙ +M =T sx(x) ˙x+M

=T sx(x)(Ax+Busyn) +M = 0 (6) Thus,

usyn=−(T sx(x)B)−1(T sx(x)Ax+M)

=ueq+us (7)

where (sx(x)B) is invertible.

ueq=−(T sxB)−1T sxAxdenotes the equivalent con- trol law that drives the state trajectories to converge toward the manifold and us = −(T sxB)−1s(x) is the smooth component that maintains the system dynamics along the manifolds.

The system dynamics along the manifoldM = 0 is given by two equations as follows:

M = 0

˙

x=Ax+Busyn

= (I−B(T sx(x)B)−1T sx(x))Ax−

B(T sx(x)B)−1M = 0

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These equations prove the advantage of the order reduc- tion of the synergetic control. It provides a reduced-order, n−m- dimensional dynamical system.

Theorem 1. Consider linear system (2) and diagonal positive definite matrix T . Using the control law that satisfies (4), the state trajectories will converge to the man- ifold and the convergence speed depends on the designated parameterT.

Proof 1. Consider the Lyapunov function defined as V(s(x)) =sT(x)s(x). Derivation ofV(s(x)) gives:

V˙(s(x)) = 2sT(x) ˙s(x) (9) From (4) we have

˙

s(x) =−T−1s(x) (10) Hence,

V˙(s(x)) =−2sT(x)T−1s(x)<0, f or T >0 (11) Thus, the stability condition is guaranteed for such syner- getic control law and the rate of convergence of the system

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state to the manifold depends onT.

It is clear from (7) that the synergetic control depends on the dynamic matrixA. Therefore, if the synergetic control is used when a fault that can change the system dynam- ics occurs, the system adapts easily to this change and compensates for the effect of the fault. This feature can be considered as an advantage used for designing resilient control when the fault caused by the system dynamics changes.

In what follows we will estimate the fault indicator using the adaptive observer.

3.2 Fault Estimation

For designing the resilient synergetic control, we need the fault indicator estimation. To this end, we will use an adaptive observer to get both the state and the fault estimations. Consider the pitch system in faulty case with a disturbance signalsddescribed by

˙

x=Ax+Bu+ ∆Af x+Ed

y=Cx (12)

where f the fault indicator is a bounded unknown scalar.

We assume that (A+ ∆Af, C) is observable for allf .Eis the distribution matrix of the disturbance. The adaptive observer is given by

˙ˆ

x=Aˆx+Bu+ ∆Afˆxˆ+K(y−y)ˆ f˙ˆ= ˆxT∆ATN(y−y)ˆ

ˆ y=Cxˆ

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Letex=x−ˆxandef=f−fˆbe the error state estimations and the error fault estimation, respectively. It follows from (12) and (13) that the estimation error system is

˙

ex= (A−KC+ ∆Af)ex+ ∆Axeˆ f+Ed f˙ˆ= ˆxT∆ATN Cex

(14) Now it is necessary to verify the stability condition of the observer. The linear matrix inequality (LMI) approach is used here to show the existence of the mentioned observer and to guarantee the estimations performance.

Theorem 2. If there exist symmetric positive definite matrixP and a full matrix X which satisfy the following condition that holds for all slow variations off .

P∆A=CTNT∆A (15)

P A−XC+P∆Af +∗ P E

ETP −µ

<0 (16) There exists an adaptive observer whose estimation errors converge to the origin via the calculation of the observer gains. Note that X =P K and thus the observer gain K is obtained as follows:

K=P−1X (17)

To minimize the estimation error [ex ef] the scalarµhas to be minimized.

Proof 2. Let the Lyapunov function be as follows:

V(t) =eTxP ex+eTfef >0 (18)

Its derivative with respect to time can be given by V˙ = 2eTxPe˙x+ 2eTff (19) where,

2eTxPe˙x= 2eTxP∆Aˆxef+ 2eTxP Ed

+2eTxP(A−KC+ ∆Af)ex (20) For all slowly varyingf , we have ˙f = 0, thus

2eTff =−2efTT∆ATN Cex (21) From (15), we can deduce

P∆Aˆx= ˆxTATfN CT

(22) We define a matrixRand scalarµsuch as:

R=P(A−KC+ ∆Af) + (A−KC+ ∆Af)TP+ 1

µP EETP (23)

Suppose that the scalar µ and the matrix P justify the following inequality:

2eTxP Ed≤ 1

µeTxP EETP ex+µkdk2 (24) Hence, we obtain

V˙ ≤eTxRex+µkdk2 (25) It follows that ˙V ≤0. This proves that the estimation error converges to a small set according to Lyapunov stability approach. Using the the Schur complement in the case of R <0 can be given otherwise.

P(A−KC+ ∆Af) +∗ P E

ETP −µ

<0 (26) where * denotes the symmetric component. Substituting P K byX and thus, the proof of the theorem is finished.

There are some difficulties in solving (15) and (16) simul- taneously to extractP andX. So, we can transform (15) into the following optimization problem:

Define the scalarη, such as η= inf

η :

ηI P ∆A−CTNT∆A

ηI

<0

(27) where * means a symmetric component.

Now it remains to design the resilient synergetic controller.

3.3 Resilient Synergetic Control

The main purpose of resilient control is to compensate for the dynamics change induced by low pressure faults in the pitch systems, so that the stability and overall closed-loop system performance can be maintained. To this purpose, we exploit the feature of the synergetic control law that depends on the system dynamics matrix A and we integrate the fault value in the system dynamics matrix.

Consider the fault-free dynamics model

˙

x=Ax+Bunom+Ed

y=Cx (28)

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After obtaining the fault indicator estimation ˆf, this estimation can be used to define a modified faulty model as follows

˙

x=Ax+Bur+ ∆Af xˆ +Ed

y=Cx (29)

where ur is the control in faulty case and unom is the nominal control.

Combining (28) and (29), the pitch system switches be- tween two models according to fault occurrence. Thus, the pitch system can be modelled as follows:

˙

x=Asx+Bus+Ed

y=Cx (30)

with,

As=A, us=unom if f < fˆ th

As=A+ ∆Af , uˆ s=ur iffˆ≥fth

(31) where fth is the threshold value of the fault indicator.

Many methods of selecting the threshold have been de- veloped (Chen and Patton [2012]). unom is the baseline controller used to achieve pitch angle control in nominal case and ur is the control used to compensate for the low pressure fault. Both controllers are designed using the synergetic control approach.

Our objective now is to construct a control strategy that not only drives the closed-loop system trajectory approaches to get the manifold s(x) = 0 but also adapts to the system dynamics change. Firstly we design the manifold using the procedure of (Slotine et al. [1991]) as follows:

s(x) = (d

dt+λ)(x1−x1ref) (32) Withλis selected by the constructer so that det ∂M∂xB

6=

0 andx1ref is a constant value representing the reference value of the first variable state x1 . This manifold leads the trajectory of the variable state x1 to converge to the reference value x1ref .

The resilient synergetic control is obtained by solving the first-order differential equation Ts(x) +˙ s(x) = 0 that is controlled by appropriately choosing the convergence parameterT . To proceed, note that

˙

s(x) =λx˙1+ ˙x2=Sx˙ (33) where S = [λ 1 ], This variable is designed so that (SB) is invertible.

The resilient control is derived from the differential equa- tion using the faulty model (29) when ˆf ≥fth as follows:

Ts(x) +˙ s(x) =T Sx˙+s(x)

= T S((A+ ∆Afˆ)x+Bur+Ed) +s(x) = 0

(34) Thus, we obtain the synergetic control law

ur=−(T SB)−1

T S(A+ ∆Afˆ)x+T SEd+s(x) (35) Hence, the obtained synergetic control comprises two terms given by

ur=−(T SB)−1(T SAx+T SEd+s(x))

−(T SB)−1∆Af xˆ

=unom+uresilient

(36)

with,

uresilient=−(T SB)−1∆Af xˆ (37) It can be seen that the resilient control depends on the additive term that represents the fault which allows to compensate for the effect of the considered fault. In fact, the designed resilient controller drives system dynamicsAs

that includes dynamics variation ∆Ato converge towards the desired performances.

The stability of the obtained controller as mentioned in the previous subsection has the simplest formT >0.

Theorem 3.The obtained controller (36) can compensate for the faultf and recover the nominal pitch dynamics.

Proof 3. The dynamics of the pitch system along the manifold in presence of fault is obtained by substituting (36) in (29) yielding

˙

x=Ax−B((T SB)−1(T SAx+T S∆Af xˆ +T SEd+s(x))) + ∆Af xˆ +Ed

=−(T S)−1s(x)

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It is clear that the pitch system dynamics along the manifold is independent of the fault, which proves that the resilient controller can compensate for the fault.

4. NUMERICAL EXAMPLE

In this section, the pitch system is used to prove the effectiveness of the proposed resilient synergetic control.

In the nominal case, we have ωn = 11.11 rad/s and ξn = 0.6 rad/s and under actuator fault, we have ωf = 3.42 rad/s and ξf = 0.9 rad/s. We suppose that there exists a measurement noise modeled by a zero mean white Gaussian noise. In this work we aim to drive the pitch angleβ to converge to the reference pitch angleβref = 6 . The synergetic control is characterized by T = 1 and λ = 6. The pitch angle β is shown in fig.2. Then, we aim to study the effect of the variation of the synergetic parameterT on the variable state evolutions (Fig.3).

0 50 100 150 200 250 300 350 400

0 1 2 3 4 5 6 7 8

Time(s)

Pitch angle

x1 xref

Fig. 2. Pitch angle

As expected, the closed loop trajectory generated by the synergetic control law converges to the manifold. In fact, the pitch angle converges to the reference value 6.

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0 50 100 150 200 250 300 350 400 1

2 3 4 5 6 7 8

Time(s)

The effect of T on the x1 evolution

T=10 T=1 T=0.1

Fig. 3. The effect of T on the evolution of the pitch angle The effect of variation of the design parameter T on the pitch system dynamics is illustrated in Fig.3. We can see from this figure that the increase of T gives a lower rate of state variable convergence toward the desired value.

So, the convergence of the system trajectories toward the manifold is inversely proportional to the value ofT . This is explained by the fact that the increase ofT is correlated with the decrease of the synergetic control law gains.

Parameters T andλcan affect stability and performance of the pitch system, thus they must be well chosen.

4.1 Resilient synergetic control

In the time period t ∈ [200; 300]s , the pitch system is affected by a drop in pressure. The fault estimation is carried out by an adaptive observer (see Fig.4). The simulation results are shown in the following figures. As

0 50 100 150 200 250 300 350 400

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

Time(s)

Fault estimation

Estimate Real

Fig. 4. Fault estimation

can be seen from Fig 4, the adaptive observer allows satisfactory fault estimation in spite of a light difference between real and estimate fault due to the noise applied to the pitch system.

Remark: We observe that the value of the synergetic parameterλaffects the fault estimation. When we increase the value of λ from 2 to 6, the fault estimation becomes more accurate and approaches the real fault. Therefore, an appropriate value of gives an adequate fault estimation.

0 50 100 150 200 250 300 350 400

−1

−0.5 0 0.5 1 1.5

Time(s)

Fault estimation

lamda=2 lamda=6

Fig. 5. Fault estimation according to the value ofλ

0 50 100 150 200 250 300 350 400

0 1 2 3 4 5 6 7 8

Time(s)

Pitch angle

xref x1

Fig. 6. Pitch angle

Fig.6 shows that in the presence of fault, the pitch angle deviates from the desired pitch angle (β 6= βref = 6, where it drops from 6 to 0.2 during the time period t ∈ [200; 300]s. In order to demonstrate the resilient control performance, the pitch angle, before and after using the synergetic resilient control, is plotted in Fig.7 and Fig.8.

0 50 100 150 200 250 300 350 400

0 1 2 3 4 5 6 7 8

Time(s)

pitch angle

x1ref

without resilient control with resiliient control

Fig. 7. Pitch angle

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0 50 100 150 200 250 300 350 400 0

2 4 6 8 10 12 14

Time(s)

resilient control

synergetic resilient control

Fig. 8. Resilient synergetic control

It can be seen from Fig.7 that the proposed resilient syner- getic control succeeded in compensating for the considered fault and recovering the pitch angle to the desired value.

The resilient control increased from 6 to 12 when the fault occurs which maintains the pitch system in the desired performance.

5. CONCLUSIONS

In this work, a fault tolerant control (FTC) system was proposed for system with fault changing system dynamics to recover the nominal operation and the desired perfor- mance. The FTC system included an adaptive observer to detect and estimate the fault and a synergetic resilient control to compensate for parameter faults. The proposed synergetic resilient control based on the synergetic theory taking into consideration the feature of dependence of the system dynamics. Finally, a numerical example proved the effectiveness of the proposed synergetic resilient control

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