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Robust stability and boundedness of uncertain conformable fractional-order delay systems under input saturation

  • In this article, a class of uncertain conformable fractional-order delay systems under input saturation is considered. By establishing the Lyapunov boundedness theorem for conformable fractional-order delay systems, some sufficient conditions for robust stability and boundedness of the systems are obtained. Examples are given to illustrate the obtained theory.

    Citation: Danhua He, Baizeng Bao, Liguang Xu. Robust stability and boundedness of uncertain conformable fractional-order delay systems under input saturation[J]. AIMS Mathematics, 2023, 8(9): 21123-21137. doi: 10.3934/math.20231076

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  • In this article, a class of uncertain conformable fractional-order delay systems under input saturation is considered. By establishing the Lyapunov boundedness theorem for conformable fractional-order delay systems, some sufficient conditions for robust stability and boundedness of the systems are obtained. Examples are given to illustrate the obtained theory.



    It is generally known that the fractional-order derivative generalizes the integer-order derivative, which attracts extensive attention for its tremendous application potentials in the domains of earthquake dynamics, electrical circuits, fluid dynamics, control theory and so forth. Compared with classical integer-order derivatives, its fractional-order counterpart can better simulate natural physical phenomena and dynamical system processes. In 2014, Khalil et al. [1] proposed a novel definition of the fractional-order derivative named conformable fractional-order derivative. It shares some advantages that neither the Caputo derivative or Riemann-Liouville derivative have. For instance, conformable fractional-order derivatives satisfy the chain rule Tα(ξη)(s)=Tαξ(η(s))Tαη(s) and the Leibniz rule Tα(ξ(s)η(s))=ξ(s)Tαη(s)+η(s)Tαξ(s), but both the Caputo derivative and the Riemann-Liouville derivative fail to provide such admirable properties.

    In the view of control, stability of fractional-order differential systems is currently a hot topic. Up to now, various meaningful and brilliant results related to stability or boundedness of fractional-order differential systems have been derived by Riemann-Liouville derivative or Caputo derivative [2,3,4,5,6,7]. Recently, Shahri et al. [8] proposed the Lyapunov method for the stability of uncertain fractional-order systems under input saturation. Advanced and interesting as their result is, the addressed systems fail to take delay effects into account. However, it is worth noting that time delays are also ubiquitous phenomenon due to some factors like limitation of transmission speed. It is reported that time delays cannot be ignored readily because the existence of delay could severely exert undesired influence on systems, which inevitably leads to instability, unboundedness, divergence, chaos, oscillation, divergence or other performance deterioration of systems [9]. On the other hand, in most practical systems, there exist many unavoidable constraints, one of which is input saturation. As a matter of fact, input saturation effects commonly exist owing to physical limitations like finite actuation power of systems. Hence, it is imperative to introduce both input saturation and delay effects into the dynamical behaviors of fractional-order differential systems. In the past decades, many differential systems with input saturation, delay effects or both have been widely investigated, and various intriguing results have been obtained [10,11,12,13,14,15,16], all of which limit the scope of the stability problem of fractional-order differential systems. However, stability may not be achieved sometimes because of some inevitable factors like external perturbations, which motivates us to further study the bounds of systems and try to confine it within a small range to realize boundedness of systems. So far, the problem with respect to the boundedness for integer-order systems has been studied widely [17,18,19]. Recently, many scholars have tried to study the boundedness of fractional-order systems, and some meaningful results have been reported [20,21,22,23]. However, most of these boundedness results are limited to the Caputo fractional-order systems. Therefore, it is necessary and meaningful to further study the boundedness problem of conformable fractional-order delay differential systems under input saturation.

    In the existing works, two techniques are widely utilized for the investigation of asymptotic behavior of fractional-order differential systems, one of which is to establish fractional-order differential inequalities. Though estimating the solution of the fractional-order differential inequalities is an effective technique to investigate the stability of fractional-order differential systems, such methods share some limitations. The other technique to study the stability of fractional-order differential systems is Lyapunov's first method and Lyapunov's second method. As we all know, Lyapunov's first method is a powerful tool for studying the asymptotic behavior of fractional-order differential systems. Lyapunov's second method is sometimes challenging to apply to a fractional-order differential system since it is by no means an easy task to compute or estimate the fractional-order derivative of the Lyapunov function in the sense of the Riemann-Liouville derivative or Caputo derivative. However, conformable fractional-order derivative enjoys some well-behaved properties, which is analogous to integer-order derivatives such that Lyapunov's second method can be applied to fractional-order differential systems more easily. Various excellent results concerning the theory and application of the fractional-order Lyapunov function are proposed in [24,25,26,27,28]. Despite this progress, boundedness analysis of conformable fractional-order delay systems under input saturation based on the Lyapunov method is still in infancy, and limited research is available on the boundedness problem of conformable fractional-order delay systems under input saturation.

    Originating from the above-mentioned discussions, this article mainly focuses on a class of uncertain conformable fractional-order delay systems under input saturation. By building the Lyapunov boundedness theorem for conformable fractional-order delayed systems, some sufficient conditions for robust stability and boundedness of the systems are obtained. Finally, numerical examples are presented to illustrate the feasibility of obtained theory. The main contributions of this article are listed as follows:

    (ⅰ) Concerned with the problem of robust stability and boundedness of conformable fractional systems and take fully into account the effects of time delays and input saturation.

    (ⅱ) Lyapunov boundedness theorem for conformable fractional-order delay systems is proposed.

    (ⅲ) Based on the Lyapunov boundedness theorem for conformable fractional-order delay systems, some sufficient conditions for robust stability and boundedness of the systems are obtained.

    The remainder of this article is organized as follows. In Section 2, some preliminaries are introduced. By establishing the Lyapunov boundedness theorem for conformable fractional-order delay systems, some sufficient conditions for robust stability and boundedness of the systems are proposed in Section 3. In Section 4, two examples are provided to illustrate the effectiveness of the main results. Finally, the conclusion is stated in Section 5.

    Let x=xTx denote the Euclidean norm of a vector x, U=eigmax(UTU) denote the trace norm of a matrix U and λmax()(λmin()) be the maximal(minimum) eigenvalue of a real symmetric square matrix.

    Definition 2.1. [1,26] For h:[s0,)R, the conformable fractional derivative starting from s0 of order α(0,1] for h is defined by

    Tαs0h(s)=limϰ0h(s+ϰ(ss0)1α)h(s)ϰ,s>s0. (2.1)

    The conformable fractional derivative at s0 is defined as Tαs0h(s0)=limss+0Tαs0h(s).

    Lemma 2.2. [26] Let h:[t0,)R be a continuous function such that Tαt0h(t) exists on (t0,), if Tαt00, for all t(t0,), then h is an increasing function.

    Lemma 2.3. [26] Let x:[t0,)Rn such that Tαt0 exists on (t0,) and Q is a symmetric positive definite matrix. Then Tαt0(xTQx) exists on (t0,) and the following relation is satisfied:

    Tαt0(xTQx)=2xTQTαt0x,t>t0. (2.2)

    Definition 2.4. [26] The conformable fractional exponential function is defined for every a0 by

    Eα(b,a)=ebaαα,

    where α(0,1] and bR.

    Lemma 2.5. [29] For any given matrices U and V with appropriate dimensions, there exists a positive scalar ϵ such that the following relationship holds:

    UTVϵ1UTV+ϵVTV. (2.3)

    In this article, we will study the following uncertain fractional-order delay system:

    Tαt0x(t)=(U+ΔU(t))x(t)+(V+ΔV(t))x(tς)+(C+ΔC(t))sat(u(t))+d(x,x(tς)), (2.4)

    where xRn denotes the state vector, U, VRn×n and CRn×m represent constant system matrices corresponding to the linear part of the system dynamics and input vector, respectively, u(t)Rm is the control input, sat():RmRm is the saturation function (its definition will be given later), and d(x,x(tς))Rn is the disturbance signal satisfying the following assumption.

    Assumption 2.6. There are three positive constants l1, l2 and l3 such that

    d(x(t),x(tς))2l1x2+l2x(tς)2ς+l3. (2.5)

    Moreover, ΔU(t)Rn and ΔV(t)Rn stand for time-varying uncertain terms regarding to the mismatch model of the linear term, and ΔC(t)Rn×m is the input matrix uncertainty satisfying the following assumption.

    Assumption 2.7. There are three positive constants α, β and γ such that

    ΔUα,ΔVβ,ΔCγ. (2.6)

    Remark 2.8. [30] A nonlinear function h() meets the Lipchitz condition if and only if

    h(y1)h(y2)Lhy1y2, (2.7)

    where Lh>0 is the Lipschitz constant and y1,y2Rn.

    Remark 2.9. [31] The saturation function denoted by sat():RmRm, sat(u)=(sat(u1),sat(u2),,sat(um))T, sat(ui)=min(ui,1)sign(ui) satisfies the Lipschitz condition.

    Remark 2.10. [32] Let KRm×n be a constant matrix, φ(x)=sat(Kx)Kx, then there is a constant lφ0 such that

    φ(x1)φ(x2)lφx1x2. (2.8)

    In this section, we will study the robust stability and boundedness of the system (2.4) via Lyapunov methods. To begin with, let us introduce the following Lyapunov boundedness theorem for conformable fractional-order delay systems.

    Theorem 3.1. Suppose that x is a solution of the conformable fractional-order delay system

    {Tαt0x=f(t,x,x(tς)),x(t0+ν)=φ(ν),ν[ς,0],φC[[ς,0],Rn]. (3.1)

    If there exist a Lyapunov function G(t,x(t)) and positive numbers ϱi (i=1,2,...,5) with ϱ1ϱ3>ϱ2ϱ4 such that

    ϱ1x2G(t,x)ϱ2x2,(t,x)[t0ς,)×Rn, (3.2)
    Tαt0G(t,x)ϱ3x2+ϱ4x(t)2ς+ϱ5,(t,x)[t0,)×Rn, (3.3)

    where [G(t,x(t))]ς=supςν0G(t+ν,x(t+ν)). Then, system (3.1) is exponentially ultimately bounded and the solution of system (3.1) obeys

    xρ2ϱ1ϕEα(ϑ2,tt0))+ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4,tt0, (3.4)

    where ϑ>0 is a solution of the following inequality:

    ϱ4ϱ1Eα(ϑ,ς)ϱ3ϱ2+ϑ<0. (3.5)

    Proof. Using (3.2) and (3.3), we have

    Tαt0G(t,x)ϱ3ϱ2G(t,x)+ϱ4ϱ1[G(t,x(t))]ς+ϱ5,(t,x)[t0,)×Rn. (3.6)

    Next, we claim that

    G(t,x)[G(t0,x(t0))]ςEα(ϑ,(tt0)0)+ϱ1ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4,t[t0ς,). (3.7)

    Let

    ζ(t)=[G(t0,x(t0))]ςEα(ϑ,(tt0)0)+ϱ1ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4,t[t0ς,). (3.8)

    If (3.7) is false, then, by Lemma 2.2, there is a t>t0 such that

    G(t,x)=ζ(t), (3.9)
    Tαt0G(t,x)Tαt0ζ(t), (3.10)
    G(t,x)ζ(t),t[t0,t). (3.11)

    According to Definition 2.1, we have

    Tαt0ζ(t)=limη0{1η[[G(t0,x(t0))]ςeϑ(t+η(tt0)1αt0)αα[G(t0,x(t0))]ςeϑ(tt0)αα]}=limη0[ϑα[G(t0,x(t0))]ςeϑ(t+η(tt0)1αt0)ααα(t+η(tt0)1αt0)α1(tt0)1α]=ϑ[G(t0,x(t0))]ςeϑ(tt0)αα(tt0)α1(tt0)1α=ϑ[G(t0,x(t0))]ςeϑ(tt0)αα,tt0. (3.12)

    Therefore, by (3.12) one has

    Tαt0ζ(t)=ϑ[G(t0,x(t0))]ςeϑ(tt0)αα. (3.13)

    It follows from (3.6), (3.8), (3.9) and (3.13) that

    Tαt0G(t,x)ϱ3ϱ2G(t,x)+ϱ4ϱ1[G(t,x(t))]ς+ϱ5[G(t0,x(t0))]ς[ϱ3ϱ2Eα(ϑ,tt0)+ϱ4ϱ1Eα(ϑ,(tςt0)0]ϱ3ϱ2ϱ1ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4+ϱ4ϱ1ϱ1ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4+ϱ5[G(t0,x(t0))]ς[ϱ3ϱ2Eα(ϑ,tt0)+ϱ4ϱ1Eα(ϑ,tt0)Eα(ϑ,ς)][G(t0,x(t0))]ς[ϱ3ϱ2+ϱ4ϱ1Eα(ϑ,ς)]Eα(ϑ,tt0)<ϑ[G(t0,x(t0))]ςEα(ϑ,tt0)Tαt0ζ(t). (3.14)

    This contradicts (3.10). Thus, one has

    G(t,x)[G(t0,x(t0))]ςEα(ϑ,tt0)+ϱ1ϱ2ϱ5ϱ1ϱ3ϱ2ϱ4,t[t0,+). (3.15)

    From this together with the condition (3.2), we know that (3.4) holds. The proof is completed.

    Corollary 3.2. Under the assumptions of Theorem 3.1, if ϱ5=0, then system (3.1) is exponentially stable and the solution of system (3.1) obeys

    xρ2ϱ1ϕEα(ϑ2,tt0)),tt0, (3.16)

    where ϑ>0 is a solution of the inequality

    ϱ4ϱ1Eα(ϑ,ς)ϱ3ϱ2+ϑ<0. (3.17)

    Proof. By Theorem 3.1, the corollary follows.

    Remark 3.3. Theorem 1 in [26] is a special case of our Corollary 3.2.

    If we consider a state feedback u=Kx,KRm×n, satisfying u0uu0, then the closed-loop system can be written as

    Tαtx=(Ucl+ΔU)x+(V+ΔV)x(tς)+Cφ(x,t)+ΔCsat(Kx)+d(x,x(tς)), (3.18)

    where Ucl=U+CK and φ(x,t)=sat(Kx)Kx.

    Remark 3.4. If 0<ui1, then the saturation function works in linear domain, sat(u)=u and the entire closed-loop system is

    Tαtx=(U+ΔU)x+(V+ΔV)x(tς)+(C+ΔC)Kx+d(x,x(tς)),Tαtx=(Ucl+ΔU+ΔCK)x+(V+ΔV)x(tς)+d(x,x(tς)). (3.19)

    Theorem 3.5. Consider the closed-loop system (3.19) with d(x,x(tς))=0 under the Assumption 2.7. If there exist positive constants ϵ1, ϵ2, ˆϱ3 with ˆϱ3>ϵ1+ϵ2 and the controller matrix K such that the following relationship is satisfied:

    Ucl+αI+γKI+ϵ12β2I+ϵ11VVT+ˆϱ3I0. (3.20)

    Then, the closed-loop system (3.19) is robustly exponentially stable and the solution obeys

    xϕEα(ϑ2,tt0)),tt0, (3.21)

    where ϑ>0 is a solution of the following inequality:

    2(ϵ1+ϵ2)Eα(ϑ,ς)2ˆϱ3+ϑ<0. (3.22)

    Proof. Let us choose the following Lyapunov function:

    G=12xTx. (3.23)

    Using Lemmas 2.3 and 2.5, we can derive that

    TαtG=xT(Ucl+ΔU+ΔCK)x+xT(V+ΔV)x(tς)xT(Ucl+ΔU+ΔCK)x+xTVx(tς)+xTΔVx(tς)xT(Ucl+ΔU+ΔCK)x+ϵ11xTVVTx+ϵ12xTΔVΔVTx+ϵ1x(tς)Tx(tς)+ϵ2x(tς)Tx(tς). (3.24)

    From Assumption 2.7 and (3.24), we have

    TαtGxT(Ucl+αI+γKI+ϵ12β2I)x+ϵ11xTVVTx+(ϵ1+ϵ2)x(tς)Tx(tς)ˆϱ3x2+(ϵ1+ϵ2)x(t)2ς. (3.25)

    Based on Corollary 3.2, the closed-loop system (3.19) with d(x,x(tς))=0 is robustly exponentially stable and the solution obeys (3.21). The proof is completed.

    Theorem 3.6. Consider the closed-loop system (3.19) under Assumptions 2.6 and 2.7. If there exist a positive symmetric definite matrix Q, the controller matrix K and positive scalars ˆϱ3, ˆϱ4 and ϵi, i=1,2,...5, such that the following relationships hold:

    Q(Ucl+αI+γKI)+(ϵ13+ϵ14+ϵ15)QQT+ϵ5l1I+ˆϱ3I0, (3.26)
    (ϵ3VTV+ϵ4β2I)+ϵ5l2Iˆϱ4I0, (3.27)
    λmin(Q)ˆϱ3λmax(Q)ˆϱ4>0. (3.28)

    Then, the closed-loop system (3.19) is robustly exponentially ultimately bounded and and the solution obeys

    xλmax(Q)λmin(Q)ϕEα(ϑ2,tt0))+λmax(Q)ϵ5l3λmin(Q)ˆϱ3λmax(Q)ˆϱ4,tt0, (3.29)

    where ϑ>0 is determined by the following inequality:

    2ˆϱ4λmin(Q)Eα(ϑ,ς)2ˆϱ3λmax(Q)+ϑ<0. (3.30)

    Proof. Let us choose the following Lyapunov function:

    G=12xTQx. (3.31)

    Clearly,

    12λmin(Q)x2G(t,x(t))12λmax(Q)x2. (3.32)

    Using Lemmas 2.3 and 2.5, we can derive that

    TαtG=xTQ((Ucl+ΔU+ΔCK)x+(V+ΔV)x(tς)+d(x,x(tς)))=xTQ((Ucl+ΔU+ΔCK)x+(V+ΔV)x(tς))+xTQd(x,x(tς))xTQ(Ucl+ΔU+ΔCK)x+xTQVx(tς)+xTQΔVx(tς)+xTQd(x,x(tς))xTQ(Ucl+ΔU+ΔCK)x+ϵ13xTQQTx+ϵ14xTQQTx+ϵ15xTQQTx+ϵ3x(tς)TVTVx(tς)+ϵ4x(tς)TΔVTΔVx(tς)+ϵ5d(x,x(tς))Td(x,x(tς)). (3.33)

    Then, using Assumptions 2.6 and 2.7, we have

    TαtGxTQ(Ucl+αI+γKI)x+(ϵ13+ϵ14+ϵ15)xTQQTx+ϵ3x(tς)TVTVx(tς)+ϵ4x(tς)TΔVTΔVx(tς)+ϵ5[l1x+l2x(tς)ς+l3]xTQ(Ucl+αI+γKI)x+(ϵ13+ϵ14+ϵ15)xTQQTx+x(tς)T(ϵ3VTV+ϵ4β2I)x(tς)+ϵ5(l1x2+l2x(tς)2ς+l3).

    This together with (3.26) and (3.27), we have

    TαtGˆϱ3x2+ˆϱ4x(tς)2ς+ϵ5l3. (3.34)

    Then, with the help of (3.28), (3.32) and (3.34), one can apply Theorem 3.1 to conclude that the closed-loop system (3.19) is robustly exponentially ultimately bounded and the solution obeys (3.29). The proof is completed.

    Theorem 3.7. Consider the closed-loop system (3.18) with d(x,x(tς))=0. Suppose that Assumption 2.7 holds. If there exist a positive symmetric definite matrix Q, the controller matrix K and positive scalars ˆϱ3, ˆϱ4 and ϵi, i=1,2,...5, such that the following relationships hold:

    QUcl+(ϵ11+ϵ12+ϵ13+ϵ15γ2)QQT+ϵ14QCCTQT+(ϵ1α2+ϵ4l2φ+ϵ5(lφ+K)2)I+ˆϱ3I0, (3.35)
    ϵ2VTV+ϵ3β2Iˆϱ4I0, (3.36)
    λmin(Q)ˆϱ3λmax(Q)ˆϱ4>0. (3.37)

    Then, the closed-loop system (3.18) with d(x,x(tς))=0 is robustly exponentially stable and the solution obeys

    xϕEα(ϑ2,tt0)),tt0, (3.38)

    where ϑ>0 is a solution of the inequality

    2ˆϱ4λmin(Q)Eα(ϑ,ς)2ˆϱ3λmax(Q)+ϑ<0. (3.39)

    Proof. Let us choose the following Lyapunov function:

    G(t,x(t))=12xTQx. (3.40)

    Using Lemmas 2.3 and 2.5, we can derive that

    TαtG=xTQ((Ucl+ΔU)x+(V+ΔV)x(tς)+Cφ(x,t)+ΔCsat(Kx))=xTQUclx+xTQΔUx+xTQVx(tς)+xTQΔVx(tς)+xTQCφ(x,t)+xTQΔCsat(Kx))xTQUclx+ϵ11xTQQTx+ϵ1xTΔUTΔUx+ϵ12xTQQTx+ϵ2x(tς)TVTVx(tς)+ϵ13xTQQTx+ϵ3x(tς)TΔVTΔVx(tς)+ϵ14xTQCCTQTx+ϵ4φ(x,t)Tφ(x,t)+ϵ15xTQΔCΔCTQTx+ϵ5sat(Kx)Tsat(Kx). (3.41)

    Then, using Assumption 2.7 and Remark 2.10, we have

    TαtGxTQUclx+ϵ11xTQQTx+ϵ1xTα2x+ϵ12xTQQTx+ϵ2x(tς)TVTVx(tς)+ϵ13xTQQTx+ϵ3x(tς)Tβ2x(tς)+ϵ14xTQCCTQTx+ϵ4xTl2φx+ϵ15xTQγ2QTx+ϵ5xT(lφ+K)2x=xT(QUcl+(ϵ11+ϵ12+ϵ13+ϵ15γ2)QQT+ϵ14QCCTQT+(ϵ1α2+ϵ4l2φ+ϵ5(lφ+K)2)I)x+x(tς)T(ϵ2VTV+ϵ3β2I)x(tς). (3.42)

    This together with (3.35) and (3.36), we have

    TαtGˆϱ3x2+ˆϱ4x(tς)2ς. (3.43)

    Based on the Corollary 3.2, the closed-loop system (3.18) with d(x,x(tς))=0 is robustly exponentially stable and the solution obeys (3.38). The proof is completed.

    Theorem 3.8. Consider the closed-loop system (3.18) under Assumptions 2.6 and 2.7. If there exist a positive symmetric definite matrix Q, the controller matrix K and positive scalars ˆϱ3, ˆϱ4 and ϵi, i=1,2,...6, such that the following relationships hold:

    QUcl+(ϵ11+ϵ12+ϵ13+ϵ16+ϵ15γ2)QQT+ϵ14QCCTQT+(ϵ1α2+ϵ4l2φ+ϵ6l1+ϵ5(lφ+K)2)I+ˆϱ3I0, (3.44)
    ϵ2VTV+ϵ3β2I+ϵ6l2Iˆϱ4I0, (3.45)
    λmin(Q)ˆϱ3λmax(Q)ˆϱ4>0. (3.46)

    Then, the closed-loop system (3.18) is robustly exponentially ultimately bounded and the solution obeys

    xλmax(Q)λmin(Q)ϕEα(ϑ2,tt0))+λmax(Q)ϵ6l3λmin(Q)ˆϱ3λmax(Q)ˆϱ4,tt0, (3.47)

    where ϑ>0 is a solution of the following inequality:

    2ˆϱ4λmin(Q)Eα(ϑ,ς)2ˆϱ3λmax(Q)+ϑ<0. (3.48)

    Proof. Let us choose the following Lyapunov function:

    G=12xTQx. (3.49)

    Using Lemmas 2.3 and 2.5, we can derive that

    TαtG=xTQ((Ucl+ΔU)x+(V+ΔV)x(tς)+Cφ(x,t)+ΔCsat(Kx)+d(x,x(tς)))=xTQUclx+xTQΔUx+xTQVx(tς)+xTQΔVx(tς)+xTQCφ(x,t)+xTQΔCsat(Kx)+xTQd(x,x(tς))xTQUclx+ϵ11xTQQTx+ϵ1xTΔUTΔUx+ϵ12xTQQTx+ϵ2x(tς)TVTVx(tς)+ϵ13xTQQTx+ϵ3x(tς)TΔVTΔVx(tς)+ϵ14xTQCCTQTx+ϵ4φ(x,t)Tφ(x,t)+ϵ15xTQΔCΔCTQTx+ϵ5sat(Kx)Tsat(Kx)+ϵ16xTQQTx+ϵ6d(x,x(tς))Td(x,x(tς)). (3.50)

    Then, using Assumptions 2.6 and 2.7, we have

    TαtGxTQUclx+ϵ11xTQQTx+ϵ1xTα2x+ϵ12xTQQTx+ϵ2x(tς)TVTVx(tς)+ϵ13xTQQTx+ϵ3x(tς)Tβ2x(tς)+ϵ14xTQCCTQTx+ϵ4xTl2φx+ϵ15xTQγ2QTx+ϵ5xT(lφ+K)2x+ϵ16xTQQTx+ϵ6(l1x2+l2x(tς)2ς+l3)=xT(QUcl+(ϵ11+ϵ12+ϵ13+ϵ16+ϵ15γ2)QQT+ϵ14QCCTQT+(ϵ1α2+ϵ4l2φ+ϵ6l1+ϵ5(lφ+K)2)I)x+x(tς)T(ϵ2VTV+ϵ3β2I+ϵ6l2I)x(tς)+ϵ6l3. (3.51)

    This together with (3.44) and (3.45), we have

    TαtGˆϱ3x2+ˆϱ4x(tς)2ς+ϵ6l3. (3.52)

    Then, with the help of (3.32), (3.46) and (3.52), one can apply Theorem 3.1 to conclude that the closed-loop system (3.18) is robustly exponentially ultimately bounded and the solution obeys (3.47). The proof is completed.

    Remark 3.9. Taking W=Q1 in Theorem 3.8, the boundedness condition becomes

    UclW+(ϵ11+ϵ12+ϵ13+ϵ16+ϵ15γ2)I+ϵ14CCT+(ϵ1α2+ϵ4l2φ+ϵ6l1+ϵ5(lφ+K)2+ˆϱ3)WIW10,ϵ2VTV+ϵ3β2I+ϵ6l2I+ˆϱ4I0,λmin(W)ˆϱ3λmax(W)ˆϱ4>0.

    Remark 3.10. Take Theorem 3.8 for example, the design procedure of the controller is as follows:

    (1) Calculate li, i=1,2,3 from Assumption 2.6, and calculate α, β and γ from Assumption 2.7.

    (2) Choose constants ϵi>0, i=1,...,6 from Lemma 2.5.

    (3) Compute QUcl, QQT QCCTQT, VTV, λmin(Q) and λmax(Q).

    (4) Choose ˆϱ4>0 which satisfies (3.45).

    (5) Choose ˆϱ4>0 which satisfies (3.46).

    (6) Select suitable controller matrix K such that (3.45) holds.

    Remark 3.11. Based on the Lyapunov method, some sufficient conditions of the stability for a class of fractional-order systems under input saturation has been derived in [8]. Obviously, their conditions cannot be used to verify the stability and boundedness of the system (2.4). In fact, the conditions in [8] are limited to stability and are not valid for boundedness. On the other hand, the conditions in [8] are limited to Caputo fractional-order systems and are not suitable for conformable fractional-order systems.

    Remark 3.12. Although some effective methods for studying stability and boundedness have been proposed for conformable fractional-order systems [26,27], these results are ineffective to investigate the stability and boundedness of (2.4) since time delays and input saturation were ignored in [26,27].

    In the current section, two examples are provided to illustrate the effectiveness of the main results.

    Example 4.1. Consider the following fractional-order delay systems:

    [T0.9t0x1T0.9t0x2]={[12.50013.5]+ΔU}[x1x2]+{[1.50.50.71.3]+ΔV}[x1(t2)x2(t2)]+{[11]+ΔC}sat(u)+d(x,x(tς)), (4.1)

    where

    ΔU=0.5[1001]sin(t),ΔV=0.2[1001]cos(t),ΔC=0.3[11]cos(t),d(x,x(tς))=0.5x+0.5x(t2)+2.

    Let Q=I2. Based on Remark 3.10, one can check that all the conditions of Theorem 3.8 are satisfied by taking ϵ1=ϵ4=ϵ6=1, ϵ2=0.5, ϵ3=10, ϵ5=0.1, ϱ3=3.55, ϑ=0.05, ϱ4=2.85 and K=[1,1]. According to Theorem 3.8, the robust exponential boundedness of closed-loop system (4.1) is reached. The time response of the closed-loop system (4.1) with initial conditions is shown in Figure 1.

    Figure 1.  The trajectories of x1 and x2 of system (4.1).

    Example 4.2. Consider the following fractional-order delay systems:

    [T0.95t0x1T0.95t0x2]={[1.5111.5]+ΔU}[x1x2]+{[0.05000.04]+ΔV}[x1(t2)x2(t2)]+{[11]+ΔC}sat(u), (4.2)

    where

    ΔU=0.05[1001]sin(t),ΔV=0.04[1001]cos(t),ΔC=0.03[11]cos(t).

    One can check that all the conditions of Theorem 3.7 are satisfied by taking Q=I2, ϵ1=ϵ2=ϵ3=10, ϵ4=0.5, ϵ5=0.1, ϱ3=0.35, ϑ=0.05, ϱ4=0.05 and K=[1,1]. According to Theorem 3.7, the robust exponential stability of the closed-loop system (4.2) is reached. The time response of the closed-loop system (4.2) with initial conditions is shown in Figure 2.

    Figure 2.  The trajectories of x1 and x2 of system (4.2).

    In this article, we considered uncertain conformable fractional-order delay systems under input saturation. The Lyapunov boundedness theorem for conformable fractional-order delay systems was proposed by the the fractional comparison principle. Using the Lyapunov boundedness theorem, some sufficient conditions for robust stability and boundedness of the systems were presented. Two examples were given to show the validity of the obtained results. Considering that time delays sometimes appear in the derivative of the state, we will extend the results of this article to the neutral case in future work.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work was supported by the National Natural Science Foundation of China (No. 11501518).

    No potential conflict of interest was reported by the author.



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