In this paper, for a regularized fuzzy system, a generalization of the direct Lyapunov method is adapted on the base of matrix-valued Lyapunov-like functions. First, the new concept of a regularization scheme for fuzzy systems is discussed and the matrix-valued Lyapunov function technique is introduced. Then, sufficient conditions are established for the boundedness and stability of the equilibrium set of solutions of the regularized fuzzy system of differential equations. Scalar and vector Lyapunov-type functions are used based on an auxiliary matrix-valued function. Finally, a discussion is offered for the future directions of the proposed approach. Since the strategies for the analysis of the stability of fuzzy models are very important in numerous aspects, we expect that our results will inspire researchers to develop the introduced concept.
Citation: Anatoliy Martynyuk, Gani Stamov, Ivanka Stamova, Yulya Martynyuk–Chernienko. On the regularization and matrix Lyapunov functions for fuzzy differential systems with uncertain parameters[J]. Electronic Research Archive, 2023, 31(10): 6089-6119. doi: 10.3934/era.2023310
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In this paper, for a regularized fuzzy system, a generalization of the direct Lyapunov method is adapted on the base of matrix-valued Lyapunov-like functions. First, the new concept of a regularization scheme for fuzzy systems is discussed and the matrix-valued Lyapunov function technique is introduced. Then, sufficient conditions are established for the boundedness and stability of the equilibrium set of solutions of the regularized fuzzy system of differential equations. Scalar and vector Lyapunov-type functions are used based on an auxiliary matrix-valued function. Finally, a discussion is offered for the future directions of the proposed approach. Since the strategies for the analysis of the stability of fuzzy models are very important in numerous aspects, we expect that our results will inspire researchers to develop the introduced concept.
One of the main assumptions in the classical stability of motion theory [1,2] is the assumption of the invariance of the parameters of a system in the course of its movement.
Further development of the stability theory is associated with the investigation of dynamical systems with uncertain parameters. See, for example, [3] and some of the references therein, as well as some recent results on models with uncertain parameters [4,5,6,7]. The active research on the stability analysis for systems with parameter uncertainties shows the importance of the topic for practice. In fact, many real-world problems exhibit different types of uncertainties. That is why there are numerous studies that have addressed the elaboration of power techniques to investigate of the effect of parameter uncertainties [8,9,10,11,12].
One of the main tools in the study of the stability behavior of different classes of systems with uncertain parameters are the scalar and vector Lyapunov-type of functions [13,14,15,16,17]. The method of matrix-valued Lyapunov functions for the stability analysis of the solutions of continuous systems of differential equations has been developed and outlined in the monographs [18,19].
Due to the benefits for theory and applications, the Lyapunov function strategy has attracted much attention from researchers of fuzzy systems of differential equations, and it is intensively applied in their stability analysis. For example, the book [20] offers an excellent overview of the state-of-the-art research on the theory of fuzzy differential equations and inclusions and provides a systematic account of the developments in their stability analysis. The stability theory for fuzzy differential equations based on Lyapunov functions has also been developed in numerous articles [21,22,23,24,25]. However, the method of matrix Lyapunov functions has not been elucidated for such systems, which is one of the main goals of this research.
In addition, for fuzzy systems with uncertain parameters, the development of new methods for the qualitative analysis of stability and boundedness remains an open problem.
In our earlier paper [26] we introduced a regularization scheme for systems of fuzzy differential equations with uncertain parameters as a new approach in the study of the properties of such systems. The proposed strategy reduces a collection of fuzzy differential equations to a simple form that allows for analysis of the properties of solutions of both the original fuzzy system of differential equations, as well as the reduced collection of differential equations. The idea is to use a family of mappings and regularize the fuzzy systems with respect to uncertain parameters.
In this paper, using the proposed approach in [26], sufficient conditions for the stability and boundedness of the equilibria of the regularized fuzzy system are proposed through the application of the Lyapunov function method on the basis of matrix-valued functions and non-linear integral inequalities. The established results contribute to the development of new methods for the study of fuzzy differential systems with uncertain parameters. This research also adopts the matrix-valued Lyapunov function strategy to their qualitative analysis.
The contributions of our paper are as follows:
(ⅰ) using a new regularization scheme for uncertain fuzzy differential equations with uncertain parameter we establish stability criteria for the regularized system via the matrix-valued Lyapunov function technique;
(ⅱ) stability analysis for autonomous comparison problems is proposed and new stability results for autonomous systems are established;
(ⅲ) boundedness and Lagrange stability criteria for the regularized system are proved;
(ⅳ) the results offered show that the regularization scheme is a very advantageous technique which allows for analysis of the qualitative properties of solutions of both the original fuzzy system of differential equations, as well as the intermediate families of differential equations in a simple way.
The investigation is organized according to the following plan. In Section 2 some important notes on fuzzy sets and functions are provided. Section 3 is devoted to the new regularization approach developed in [26]. Matrix-valued Lyapunov functions and some of their properties are considered in Section 4. In Section 5 stability, uniform stability and asymptotic stability results for the regularized system are established. In Section 6, a stability analysis for autonomous comparison problems is conducted. Section 7 includes the boundedness results. Finally, Section 8 offers some comments and future directions for research.
We assume that X is a basic set, and that, for any x∈X, φ(x) is a membership function that takes its values from the interval [0,1]. Following [27,28,29] for a fuzzy set with a membership function φ on X its κ-level sets [φ]κ are defined as
[φ]κ={x∈X: φ(x)≥κ}, κ∈(0,1] |
and its support is given by
[φ]0=¯⋃κ∈(0,1][φ]κ. |
We will use the following notation for the Hausdorff distance between two sets Ξ,Π∈Rn and Ξ,Π≠∅:
dH(Ξ,Π)=min{H≥0:Ξ⊆{Π∪ΠH(0)}, Π⊆{Ξ∪ΠH(0)}}, |
where ΠH(0)={x∈Rn:‖x‖<H}, H≥0.
The defined Hausdorff distance dH(Ξ,Π) is a metric for any nonempty closed sets in Rn. In addition, the pair (Cn,dH) is a metric space, where Cn is the set of all nonempty closed sets in Rn.
We will denote by En the space of all functions φ:Rn→[0,1] such that
1) φ is upper semicontinuous in the sense of Baire;
2) there exists an x0∈Rn such that φ(x0)=1;
3) u is fuzzy convex, i. e., φ(λx+(1−λ)y)≥min{φ(x),φ(y)}, λ∈[0,1];
4) the closure of the set {x∈Rn:φ(x)>0} is a compact subset of Rn.
It is well known [20,26,29] that, if a fuzzy set with a membership function φ is a fuzzy convex set, then [φ]κ is convex in Rn for any κ∈[0,1].
The distance between two sets φ,ϖ∈En will be given as d(φ,ϖ)=sup{|φ(x)−ϖ(x)|: x∈Rn}; also, the least upper bound of the metric d on the space En is defined by d[φ,ϖ]=sup{dH([φ]κ,[ϖ]κ): κ∈[0,1]} for φ,ϖ∈En, and it is a metric in En.
For any two sets φ,ϖ∈En the element ι∈En such that φ=ϖ+ι, which, if it exists, is the Hukuhara difference of φ and ϖ and is denoted by φ−ϖ.
The family of all nonempty compact convex subsets of Rn will be denoted by Pk(Rn).
The integral of a mapping F on a compact interval T=[t1,t2], t2>t1>0 is denoted by b∫aF(t)dt; for any 0<κ≤1, it is given as
∫TF(t)dt={∫Tˉf(t)dt∣ˉf: T→Rn is a measurable selection forFκ}. |
The mapping F:T→En is said to be differentiable at t0∈T if the value F′(t0) exists and F′(t0)∈En is such that both limits lim{[F(t0+h)−F(t0)]h−1:h→0+} and lim{[F(t0)−F(t0−h)]h−1:h→0+} exist and are equal to F′(t0). The above limits are considered in the metric space (En,d).
If Fκ is differentiable, the mapping Fκ is differentiable in the sense of Hukuhara for all κ∈[0,1] and DHFκ(t)=[F′(t)]κ, where DHFκ is the Hukuhara-type derivative of Fκ.
The family {DHFκ(t):κ∈[0,1]} determines an element F′(t)∈En. Also, if F:T→En is differentiable at t∈T, then the element F′(t) is called the fuzzy derivative of F(t) at the point t.
More on the concepts of fuzzy sets and functions is available in [30,31,32] and some of the references therein. For important results related to fuzzy differential equations, see [33,34,35,36,37].
Throughout the entire paper we consider the following fuzzy system with an uncertain parameter
dudt=f(t,u,α),u(t0)=u0, | (3.1) |
where u∈En2; f∈C(R+×En2×S,En2); En2=En×En; α∈S is an uncertain parameter; S is a compact set in Rd.
{As it is stated in [26], the parameter vector α represents the uncertainty in system (3.1). It can have a different nature and may represent different characteristics. For example, the uncertainty parameter α
(a) may describe an uncertain value of a certain physical parameter;
(b) may represent an estimate of an external disturbance;
(c) may describe an inaccurate measured value of the input effect of one of the subsystems on the other one;
(d) may represent some nonlinear elements of the considered mechanical system that are too complicated to be measured accurately;
(e) may be an indicator of the existence of some inaccuracies in the system (3.1);
(f) may be a union of the characteristics (a)–(e).
To regularize the system (3.1) with respect to the uncertain parameter α, in [26] we consider a family of mappings fκ(t,v) defined by
fκ(t,v)=fM(t,v)κ+(1−κ)fm(t,v),0≤κ≤1, | (3.2) |
where
fm(t,v)=¯co⋂α∈Sf(t,v,α),S⊆Rd, | (3.3) |
fM(t,v)=¯co⋃α∈Sf(t,v,α),S⊆Rd. | (3.4) |
Now, we propose to consider the following regularized with respect to α∈S system of fuzzy differential equations of the type
dvdt=fκ(t,v),v(t0)=v0, | (3.5) |
where fκ∈C(I×En2,En2), I=[t0,t0+τ], t0≥0, τ>0, κ∈[0,1].
For the regularized system (3.5) we assume that fm(t,v), fM(t,v)∈C[R+×En2,En2]. The solutions of the initial value problem (IVP) (3.5) are weakly continuous mappings v: I→En2 which satisfy the integral equation
v(t)=v0+t∫t0fκ(s,v(s))ds, t∈I, κ∈[0,1]. |
The proposed regularization scheme is a method that can help to reduce the analysis of the properties of the fuzzy system (3.1) with the uncertain parameter α∈S to those of the regularized system (3.5).
We define a matrix-valued function
U(t,⋅)=[uij(t,⋅)],i,j=1,2, | (4.1) |
with entries uij∈R that correspond to the family of regularized equations (3.5) as follows:
1) If κ=0, then the entry u11(t,v1)∈C(R+×En2, R+) corresponds to the fuzzy equation
dv1dt=fm(t,v1); | (4.2) |
2) If κ=1, then u22(t,v2)∈C(R+×En2, R+) corresponds to the fuzzy equation
dv2dt=fM(t,v2); | (4.3) |
3) If 0<κ<1, then the entries u12(t,v)=u21(t,v)∈C(R+×En2, R) correspond to the fuzzy regularized system
dvdt=fκ(t,v), | (4.4) |
where fκ∈C(R+×En2, En2).
This way the fuzzy equations (4.2)–(4.4) become the base in the construction of the matrix-valued Lyapunov-type function (4.1).
Example 4.1. As a very simple example of a matrix-valued Lyapunov function, consider a function U(t,⋅) with the following entries:
u11(t,v1)=d[v1,θ0]; u22(t,v2)=d[v2,θ0]; u12(t,v1,v2)=u21(t,v1,v2)=d[v1,v2], |
where v1,v2∈En2 and the state θ0∈En2 is defined as
θ0(x)={1,forx=0,0,forx∈Rn∖{0}. |
Now, on the basis of the matrix function (4.1), and by means of a vector η∈R2+, we construct a scalar Lyapunov-type function as follows
V(t,v,η)=ηTU(t,v)η, | (4.5) |
where V∈C(R+×En2×R2+, R+).
Note that, in general, the vector η can be defined in one of the following ways:
(a) η=y∈R2, y≠0;
(b) η=ξ∈C(R2, R2+), ξ(0)=0;
(c) η=ψ∈C(R+×R2, R2+), ψ(t,0)=0;
(d) η∈R2+, η>0.
Together with the defined scalar function (4.5), we will also use the following vector function, given by
L(t,v,η)=AU(t,v)η, | (4.6) |
where A is a constant (2×2) matrix, L=(L1,L2)T and L∈C(R+×En2×R2+, R2+).
We will introduce the following concepts related to the function (4.1) based on the function (4.5).
Definition 4.2. The matrix-valued function U:R+×En2→R2 is said to be
1) positive semi-definite if there exist a neighborhood D(ρ) of the state θ0, D(ρ)={v∈En2:d[v,θ0]<ρ}, 0<ρ<+∞ and a vector η∈R2+ such that
(a) the function V(t,v,η) is continuous on R+×D(ρ)×R2+;
(b) the function V(t,v,η) is nonnegative for all (t,v,η)∈R+×D(ρ)×R2+;
(c) V(t,0,η)=0 for all t∈R+ and η∈R2+;
2) positive definite if it is positive semi-definite and there exists a positive definite function w(v):D(ρ)→R+ such that w(v)≤V(t,v,η) for all (t,v,η)∈R+×D(ρ)×R2+;
3) decreasing if there exists a positive definite function z(v):D(ρ)→R+, such that V(t,v,η)≤z(v) for all (t,v,η)∈R+×D(ρ)×R2+;
4) radially unbounded if d[v,θ0]→∞ implies that V(t,v,η)→+∞ for all t∈R+ and η∈R2+.
The notions of negative semi-definite and negative definite matrix-valued functions can be defined analogously.
Together with the consideration of Lyapunov-type functions (4.5) and (4.6), we will also introduce their total derivatives with respect to the regularized system (3.5), as follows:
D+V(t,v,η)=ηTD+U(t,v)η; |
D+L(t,v,η)=AD+U(t,v)η, |
where D+U(t,v)=limsup{[U(t+h, v+hfκ(t,v))−U(t,v)]h−1:h→0+}.
Example 4.3. For the function considered in Example 4.1,
U(t,v)=(d[v1,θ0]d[v1,v2]d[v1,v2]d[v2,θ0]) |
we have
D+U(t,v)=(D+d[v1,θ0]D+d[v1,v2]D+d[v1,v2]D+d[v2,θ0]), |
where
D+d[v1,θ0]=limh→0+sup1h{d[v1+hfm(t,v1),θ0]−d[v1,θ0]}; |
D+d[v2,θ0]=limh→0+sup1h{d[v2+hfM(t,v2),θ0]−d[v2,θ0]}; |
D+d[v1,v2]=limh→0+sup1h{d[v1+hfm(t,v1), v2+hfM(t,v2)]−d[v1,v2]}. |
The application of the function U(t,v) and its total derivative allows for the investigation of the dynamical properties of the fuzzy system with uncertain parameters, as given by (3.1) on the basis of the simple fuzzy equations (4.2)–(4.4).
In this subsection, we will consider the family of regularized equations (3.5) for (t,v)∈R+×D(ρ). Let fκ∈C(R+×D(ρ),En2) for any κ∈[0,1] and the solution v(t) of the IVP (3.5) be defined on [t0,∞). For the regularized system (3.5), we will present a scalar comparison principle by using the function (4.5).
Theorem 4.4. Suppose that for the regularized system (3.5) there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that
1) The function V(t,v,η)∈C(R+×D(ρ)×R2+,R+) and there exists a constant L>0 such that
|V(t,v1,η)−V(t,v2,η)|≤Ld[v1,v2], v1,v2∈D(ρ), t∈R+, η∈R2+; |
2) There exists a function g(t,ω), g∈C(R2+,R) such that, for any κ∈[0,1]
D+V(t,v,η)≤g(t,V(t,v,η)), (t,v,η)∈R+×D(ρ)×R2+; |
3) The maximal solution rM(t;t0,ω0) of the scalar comparison equation
dωdt=g(t,ω),ω(t0)=ω0 | (4.7) |
exists on [t0,∞).
Then, V(t0,v0,η)≤ω0 implies that
V(t,v(t),η)≤rM(t;t0,ω0), t∈[t0,∞). |
Proof. Since the solution v(t) of the IVP (3.5) is defined on [t0,∞), for t∈[t0,∞), we set m(t)=V(t,v(t),η) so that m(t0)≤ω0 and evaluate the difference m(t+h)−m(t) for a sufficiently small h>0. We have that
m(t+h)−m(t)=V(t+h,v(t+h),η)−V(t,v(t),η)=V(t+h,v(t+h),η) |
−V(t+h,v(t)+hfκ(t,v(t)),η)+V(t+h,v(t) |
+hfκ(t,v(t)),η)−V(t,v(t),η)≤Ld[v(t+h),v(t)+hfκ(t,v(t))] |
+V(t+h,v(t)+hfκ(t,v(t)),η)−V(t,v(t),η), κ∈[0,1]. |
From the above estimate, we obtain
D+m(t)=limh→0+sup1h[m(t+h)−m(t)]≤D+V(t,v(t),η)+Llimh→0+sup{d[v(t+h),v(t)+hfκ(t,v(t))]}. | (4.8) |
Let v(t+h)=v(t)+z(t), where z(t) is the Hukuhara difference for a sufficiently small h>0. According to the properties of the metric d[u,v], we get
d[v(t+h),v(t)+hfκ(t,v(t))]=d[v(t)+z(t),v(t)+hfκ(t,v(t))] |
=d[z(t),hfκ(t,v(t))]=d[v(t+h)−v(t),hfκ(t,v(t))], |
and, hence
1hd[v(t+h),v(t)+hfκ(t,v(t))]=d[v(t+h)−v(t)h,fκ(t,v(t))]. | (4.9) |
Taking the limit in (4.9), we obtain
limh→0+sup1h{d[v(t+h),v(t)+hfκ(t,v(t))]}=limh→0+sup1h{d[v(t+h)−v(t)h,fκ(t,v(t))]}=d[dv(t)dt,fκ(t,v(t))] | (4.10) |
along any solution v(t) of (3.5).
Taking into account (4.10), the estimate (4.8) takes the following form:
D+m(t)≤g(t,m(t)),m(t0)≤ω0, | (4.11) |
to which we apply Theorem 1.5.1 [14] and get
m(t)≤rM(t;t0,ω0) |
for all t≥t0. This proves Theorem 4.4.
We will now state some corollaries of Theorem 4.4. The Hahn class K of continuous and strictly increasing functions of the corresponding dimension that are zero at zero will be used [14].
Corollary 4.5. Suppose that, in Theorem 4.4, instead of condition 2, we have the following:
2′) D+V(t,v,η)≤0, (t,v,η)∈R+×D(ρ)×R2+.
Then,
V(t,v(t),η)≤V(t0,v0,η), t≥t0. |
Corollary 4.6. Suppose that, in Theorem 4.4, instead of condition 2, we have the following:
2″) D+V(t,v,η)≤−a(ω(t,v))+g(t,V(t,v,η)), (t,v,η)∈R+×D(ρ)×R2+,
where ω∈C(R+×D(ρ),R+), a∈K and g(t,ω) is a function decreasing on ω for any t∈R+.
Then, V(t0,v0,η)≤ω0 implies that
V(t,v(t),η)+t∫t0a[ω(s,v(s))]ds≤rM(t;t0,ω0), t≥t0, κ∈[0,1]. |
We represent the regularized system (3.5) in the following form:
dvdt=Aκ(t)v+gκ(t,v), | (4.12) |
v(t0)=v0, | (4.13) |
where gκ∈C(R+×En2) and Aκ(t):[t0,∞)→En2 for any value of κ∈[0,1] is a semi-linear operator such that
(a) Aκ(t)(u+v)=Aκ(t)u+Aκ(t)v, u,v∈En2;
(b) Aκ(t)(νu)=νAκ(t)u, ν∈R+, u∈En2.
Assume that the solution of the problem described by (4.12) and (4.13) is well defined for t≥t0 and the operator Aκ(t) is contracting, i.e., there exists 0<γ<1 such that
d[Aκ(t)u, Aκ(t)v]≤γd[u,v], u,v∈En2. | (4.14) |
In addition, for a sufficiently small h>0 the operator
Q(h,Aκ(t))=I+hAκ(t)+h2A2κ(t)+…+hnAnκ(t)+… |
exists for t∈R+, κ∈[0,1] and u∈En2, and it satisfies
limh→0Q(h,Aκ(t))u=u. | (4.15) |
The comparison principle for the quasilinear regularized problem described by (4.12) and (4.13) is represented as follows.
Theorem 4.7. Suppose that for the regularized system (4.12), there exists a scalar Lyapunov-type function V(t,v,η) that satisfies the following conditions:
1) V(t,v,η)∈C(R+×D(ρ)×R2+,R+) and there exists a continuous on R+ function L(t)≥0 such that
|V(t,v1,η)−V(t,v2,η)|≤L(t)d[v1,v2], v1,v2∈D(ρ), t∈R+, η∈R2+; |
2) There exists a function G(t,ω), G∈C(R2+,R), such that for any κ∈[0,1]
D+V(t,v,η)≤G(t,V(t,v,η)), (t,v,η)∈R+×D(ρ)×R2+; |
3) The maximal solution rM(t;t0,ω0) of the comparison equation
dωdt=G(t,ω),ω(t0)=ω0 | (4.16) |
exists on [t0,∞).
Then, V(t0,v0,η)≤ω0 implies that
V(t,v(t),η)≤rM(t;t0,ω0), t∈[t0,∞). | (4.17) |
The proof of Theorem 4.7 is obtained in a similar way as the proof of Theorem 4.4 taking into account the fact that
Q(h,Aκ(t))v+hgκ(t,v)=v+hgκ(t,v)+h(Q(h,Aκ(t))v. | (4.18) |
From (4.18), we have the following for m(t)=V(t,v(t),η):
m(t+h)−m(t)≤L(t+h)d[v(t+h), v(t)+h(Aκ(t)v(t)+gκ(t,v(t)))] |
+L(t+h)hd[Q(h,Aκ(t))Aκ(t)v(t), Aκ(t)v(t)]+V(t+h, Q(h,Aκ(t))v(t) |
+hgκ(t,v(t)),η)−V(t,v(t),η), κ∈[0,1]. |
The above estimate, (4.14), (4.15) and condition 2 of Theorem 4.7 yield
D+m(t)≤G(t,m(t)). | (4.19) |
Next, we apply Theorem 3.1.1 [14] to obtain (4.17).
Corollary 4.8. Suppose that, in Theorem 4.7, the functions V(t,v,η)=d[v,θ0] and G=G(t,d[v,θ0]), t∈R+, v∈En2, η∈R2+, where θ0∈En2 is the state defined in Example 4.1.
Then, d[v0,θ0]≤ω0 implies that
d[v(t),θ0]≤rM(t;t0,ω0), t≥t0, κ∈[0,1]. |
Recall that a function G(t,ω), G:R+×R2+→R2 is quasimonotonic with respect to its second variable ω if ω1≤ω2 and ωi1=ωi2 for 1≤i≤2 imply that G(t,ω1)≤G(t,ω2) for any two ω1,ω2∈R2+ and t∈R+.
In the case that G(t,ω)=Aω, where A is a (2×2) matrix with entries aij, the function G(t,ω) is quasimonotonic if aij≥0 for i≠j.
Theorem 4.9. Suppose that, for the regularized system (3.5), there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.6) satisfies the following conditions:
1) L(t,v,η)∈C(R+×D(ρ)×R2+,R2+) and there exists a constant L>0 such that
||L(t,v1,η)−L(t,v2,η)||≤L||D[v1,v2]||, v1,v2∈D(ρ), t∈R+, η∈R2+, |
where D[v1,v2]=(d[v1,u1],d[v2,u2])T and ||.|| is the vector norm in R2;
2) There exists a quasimonotonic with respect to ω function G(t,ω)∈C(R+×R2+,R2), G(t,0)=0, such that, for any κ∈[0,1],
D+L(t,v,η)≤G(t,L(t,v,η)), (t,v,η)∈R+×D(ρ)×R2+; | (4.20) |
3) The maximal solution rM(t;t0,ω0) of the vector comparison equation
dωdt=G(t,ω),ω(t0)=ω0 | (4.21) |
exists on [t0,∞).
Then, L(t0,v0,η)≤ω0 implies that
L(t,v(t),η)≤rM(t;t0,ω0), t∈[t0,∞), κ∈[0,1]. |
The proof of Theorem 4.9 is similar to that of Theorem 4.4, so we omit it here.
Corollary 4.10. Suppose that, in Theorem 4.9, the function G=G(t,ω)=Aω, t∈R+, where A is a (2×2) matrix with entries aij≥0 for i≠j.
Then,
L(t,v(t),η)≤L(t0,v0,η)eA(t−t0), t≥t0, κ∈[0,1]. |
Recall that the function diam[u(t)]κ is nondecreasing as t→∞. Hence, the direct application of the metric ‖u(t)‖ in the stability analysis of the regularized system (3.5) is not suitable for its dynamical properties. For this reason, in our research we will introduce the following assumptions:
H1. For any value of the uncertain parameter α∈S the system (3.5) has a steady state θ0 such that fκ(t,θ0)=θ0 for all t∈[t0,∞).
H2. For the initial value v0∈En2 and any y0∈En2 there exists a Hukuhara difference v0−y0=w0.
H3. The solution v(t)=v(t;t0,v0) of (3.5) exists for all t≥t0 and is unique for any κ∈[0,1].
Next, we introduce the following stability notions for the steady state θ0.
Definition 5.1. The state θ0 of (3.5) is:
S1 equi-stable if, for any t0∈R+ and ε>0 there exists δ=δ(ε,t0) such that for any initial data v0∈En2 with d[v0,θ0]<δ we have that d[v(t;t0,v0),θ0]<ε for all t≥t0 and all κ∈[0,1];
S2 uniformly stable if δ in S1 does not depend on t0;
S3 quasi-equi-asymptotically stable if for any t0∈R+ and any ξ>0 there exist δ0(t0,ξ)>0 and τ(t0,ξ)∈R+ such that d[v0,θ0]<δ0(t0,ξ) implies that d[v(t;t0,v0),θ0]<ξ for all t≥t0+τ(t0,ξ) and κ∈[0,1];
S4 uniformly quasi-asymptotically stable if δ0 and τ in S3 are independent on t0;
S5 equi-asymptotically stable if S1 and S3 hold simultaneously;
S6 uniformly asymptotically stable if S2 and S4 hold simultaneously;
S7 uniformly exponentially stable if for an arbitrary solution v(t;t0,v0), we have
d[v(t),θ0]≤β(d[v0,θ0])exp[−λ(t−t0)], |
where β(d):[0,R]→R+ is nondecreasing on d for some R>0 and λ>0 is a constant.
Example 5.2. Consider on E2 the following fuzzy equation
dvdt=μv,v(0)=v0∈E2, | (5.1) |
where (μ≠0)∈[−1,1], μ=μ(κ), which we represent as follows:
{dv1dt=μv2,v2=v20,dv2dt=μv1,v1=v10 | (5.2) |
for κ∈[0,1]. At the same time, for an initial value v0∈E2 on the level [v0]κ=[v10,v20]κ for κ∈[0,1] the general solution of (5.2) has the form
{[v1(t)]κ=12(v10+v20)eμt+12(v10−v20)e−μt,[v2(t)]κ=12(v10+v20)eμt−12(v10−v20)e−μt | (5.3) |
for all 0≤κ≤1 and t≥0.
It follows from (5.3) that at all κ-levels, the zero solution of (5.1) is unstable, even for sufficiently small values of v10, v20 for any κ∈[0,1]. At the same time, the zero solution is stable under some additional conditions for the initial data [v0]κ=[v10,v20]κ. Particularly, if v10+v20=0 for 0<μ<1 or if v10−v20=0 for −1<μ<0, and any κ∈[0,1], the relations given by (5.3) imply that [v1(t)]κ and [v2(t)]κ are decreasing for t→∞. These conditions are equivalent to the existence of the Hukuhara difference for [v10,v20]κ, κ∈[0,1].
We will now establish some stability criteria for the stationary state θ0 of (3.5) based on a scalar auxiliary function of the type (4.5). Functions of the class CK={a∈C[R2+,R+]:a(t,u)∈K for each t∈R+ and a(t,℘)→∞ as ℘→∞} will also be used.
Theorem 5.3. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, and that there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.5) satisfies the following conditions:
1) V(t,v,η) satisfies condition 1 of Theorem 4.4;
2) There exist functions a∈K and b∈CK and constant positive definite (2×2) matrices A1 and A2 such that
aT(d[v,θ0])A1a(d[v,θ0])≤V(t,v,η)≤bT(t,d[v,θ0])A2b(t,d[v,θ0]) | (5.4) |
for (t,v,η)∈R+×D(ρ)×R2+;
3)
D+V(t,v,η)≤0, (t,v,η)∈R+×D(ρ)×R2+. |
Then the state θ0 of (3.5) is equi-stable.
Proof. Under the condition 2) of Theorem 5.3, the estimate (5.4) can be represented as
λm(A1)¯a(d[v,θ0])≤V(t,v,η)≤λM(A2)¯b(t,d[v,θ0]) | (5.5) |
for (t,v,η)∈R+×D(ρ)×R2+, where λm(A1)>0 and λM(A2)>0 are the minimal and maximal eigenvalues of the matrices A1 and A2, respectively, and the comparison functions ¯a∈K, ¯b∈CK exist such that
¯a(d[v,θ0])≤aT(d[v,θ0])a(d[v,θ0]) |
and
¯b(t,d[v,θ0])≥bT(t,d[v,θ0])b(t,d[v,θ0]). |
Let 0<ε<ρ and t0∈R+ be given. We choose δ=δ(t0,ε) so that
λM(A2)¯b(t0,δ)<λm(A1)¯a(ε). | (5.6) |
We will show that, for such a choice of δ, the stationary state θ0 of (3.5) is equi-stable. If this is not true, then there exist a solution v∗(t;t0,v0) and a t1>t0 such that, for κ∈[0,1],
d[v∗(t1),θ0]=εandd[v∗(t),θ0]≤ε<ρ, t0≤t<t1. | (5.7) |
According to condition 3 of Theorem 5.3 and Corollary 4.5, we have
V(t,v∗(t),η)≤V(t0,v0,η)for allt0≤t≤t1 and κ∈[0,1]. | (5.8) |
Hence, taking into account the estimates (5.5) and (5.6), we get
λm(A1)¯a(ε)=λm(A1)¯a(d[v∗(t1),θ0])≤V(t1,v∗(t1),η)≤V(t0,v0,η) |
≤λM(A2)¯b(t0,d[v0,θ0])<λm(A1)¯a(ε). |
The obtained contradiction shows that d[v0,θ0]<δ implies that d[v(t;t0,v0),θ0]<ε for all t≥t0 and all κ∈[0,1], which proves the theorem.
Theorem 5.4. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, there exists a function of the type (4.5) for which conditions 1 and 2 of Theorem 5.3 are satisfied and, instead of 3 we have the following:
3′) There exists a constant β>0 such that
D+V(t,v,η)≤−βV(t,v,η), (t,v,η)∈R+×D(ρ)×R2+. |
Then, the state θ0 of (3.5) is equi-asymptotically stable.
Proof. Since the conditions of Theorem 5.4 follow from the conditions of Theorem 5.3, the steady state θ0 is equi-stable.
Let ε=ρ and δ0=δ0(t0,ρ). From Theorem 5.3, we have that d[v0,θ0]<δ0 implies that d[v(t),θ0]<ρ for all t≥t0 and κ∈[0,1].
From condition 3′ of Theorem 5.4, we obtain
V(t,v(t),η)≤V(t0,v0,η)exp[−β(t−t0)], t≥t0, κ∈[0,1]. |
For the given ε>0 we choose
τ(t0,ε)=1βlnλM(A2)¯b(t0,δ0)λm(A1)¯a(ε)+1. |
Hence, for any κ∈[0,1]
λm(A1)¯a(d[v(t),θ0])≤V(t,v(t),η) |
≤λM(A2)¯b(t0,δ)exp[−β(t−t0)]<λm(A1)¯a(ε), t≥t0+τ(t0,ε). |
From the above inequalities, for any initial data v0∈En2 with d[v0,θ0]<δ0, we have that d[v(t;t0,v0),θ0]<ε for t≥t0+τ(t0,ε) and any κ∈[0,1], which proves Theorem 5.4.
Theorem 5.5. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, and that there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.5) satisfies the following conditions:
1) V(t,v,η) satisfies condition 1 of Theorem 4.4 on R+×(D(ρ)∩Dc(σ))×R2+, where Dc(σ) is the complement of D(σ) for 0<σ<ρ;
2) V(t,v,η) satisfies condition 2 of Theorem 5.3 on R+×(D(ρ)∩Dc(σ))×R2+ for the functions a,b∈K;
3) V(t,v,η) satisfies condition 3 of Theorem 5.3 on R+×(D(ρ)∩Dc(σ))×R2+.
Then the state θ0 of (3.5) is uniformly stable.
Proof. Condition 2) of Theorem 5.5 leads to
λm(A1)¯a(d[v,θ0])≤V(t,v,η)≤λM(A2)¯b(d[v,θ0]), (t,v,η)∈R+×(D(ρ)∩Dc(σ))×R2+. |
Let 0<ε<ρ and t0∈R+ be given. We can choose δ=δ(ε)>0 so that
λM(A2)¯b(δ)<λm(A1)¯a(ε). | (5.9) |
We will show that for the above choice of δ>0 the stationary state θ0 of the regularized system (3.5) is uniformly stable. If this is not true, then there exist a solution v(t) of (3.5) and t1,t2, where t2>t1>t0, such that d[v(t1),θ0]=δ, d[v(t2),θ0]=ε and δ≤d[v(t),θ0]≤ε<ρ for t∈[t1,t2] and κ∈[0,1].
Set σ=δ, and, according to the condition 3 of Theorem 5.5, we have
V(t2,v(t2),η)≤V(t1,v(t1),η). |
From the above inequality, we get
λm(A1)¯a(ε)=λm(A1)¯a(d[v(t2),θ0])≤V(t2,v(t2),η)≤V(t1,v(t1),η) |
≤λM(A2)¯b(d[v(t1),θ0])=λM(A2)¯b(δ)<λm(A1)¯a(ε). |
The obtained contradiction proves Theorem 5.5.
Theorem 5.6. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, there exists a function of the type (4.5) for which conditions 1 and 2 of Theorem 5.5 are satisfied and, instead of 3 we have the following:
3″) There exists a function c∈K such that
D+V(t,v,η)≤−c(d[v,θ0]), (t,v,η)∈R+×(D(ρ)∩Dc(σ))×R2+. |
Then, the state θ0 of (3.5) is uniformly asymptotically stable.
Proof. Since all conditions of Theorem 5.5 are satisfied, the state θ0 of (3.5) is uniformly stable. Then, for ε=ρ and δ0=δ0(ρ), d[v0,θ0]<δ0 implies that d[v(t),θ0]<ρ for all t≥t0 and κ∈[0,1].
To prove Theorem 5.6, we have to show that the state θ0 is attractive, i.e., that there exists a t∗≥t0 such that d[v(t∗),θ0]<δ for t0≤t∗≤t0+τ, where τ=1+λM(A2)¯b(δ0)λm(A1)¯a(δ).
Suppose that the above is not true and δ≤d[v(t),θ0] for t0≤t≤t0+τ. Then, it follows from 3″ that
V(t,v(t),η)≤V(t0,v0,η)−t∫t0c(d[v(s),θ0])ds, t0≤t≤t0+τ. |
From the last inequality for the given choice of τ, we have
0≤V(t0+τ,v(t0+τ),η)≤λM(A2)¯b(δ0)−c(δ)τ<0. |
The obtained contradiction proves that d[v0,θ0]<δ implies that d[v(t;t0,v0),θ0]<ε for t≥t0+τ, i.e., the state θ0 is attractive. Theorem 5.6 is proved.
In the next result, we will need the following concept.
Definition 5.7. Two functions a,b∈K are said to be of the same order of magnitude if there exist positive constants k1 and k2 such that k1a(r)≤b(r)≤k2a(r) for all r∈R+.
Theorem 5.8. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, and that there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.5) satisfies the following conditions:
1) V(t,v,η) satisfies condition 1 of Theorem 4.4;
2) There exist a comparison function σ1∈K, a positive constant Δ1 and a (2×2) matrix function F1(θ), θ∈R such that
Δ1dρ[v,θ0]≤V(t,v,η)≤σT1(d[v,θ0])F1(θ)σ1(d[v,θ0]) |
for (t,v,η)∈R+×D(ρ)×R2+ and ρ>1;
3) There exists a comparison function σ2∈K and a (2×2) matrix function F2(θ), θ∈R such that
D+V(t,v,η)≤σT2(d[v,θ0])F2(θ)σ2(d[v,θ0]), (t,v,η)∈R+×D(ρ)×R2+. |
Then, if the matrix F1(θ)(θ≠0)∈R2+ is positive definite, the matrix F2(θ)(θ≠0)∈R2+ is negative definite and the comparison functions σ1,σ2 are of the same order of magnitude, the state θ0 of (3.5) is uniformly exponentially stable.
Proof. We can represent the upper estimate of V(t,v,η) in condition 2) of Theorem 5.8 as follows
V(t,v,η)≤λM(F1)σT1(d[v,θ0])σ1(d[v,θ0]), | (5.10) |
where λM(F1)>0 is the maximal eigenvalue of the matrix F1.
Since the function σ1∈K, there exists a function γ∈K such that
γ(d[v,θ0])≥σT1(d[v,θ0])σ1(d[v,θ0]). | (5.11) |
From (5.10) and (5.11), it follows that condition 2 of Theorem 5.8 takes the following form:
Δ1dρ[v,θ0]≤V(t,v,η)≤λM(F1)γ(d[v,θ0]), (t,v,η)∈R+×D(ρ)×R2+. | (5.12) |
We represent condition 3 of Theorem 5.8 in the following form:
D+V(t,v,η)≤λM(F2)π(d[v,θ0]), | (5.13) |
where the function π∈K exists such that
π(d[v,θ0])≥σT2(d[v,θ0])σ2(d[v,θ0]). |
Since the functions γ and π are of the same order of magnitude, there exist constants K1>0 and K2>0 such that
K1γ(d[v,θ0])≤π(d[v,θ0])≤K2γ(d[v,θ0]). | (5.14) |
From (5.12) and (5.13) for any κ∈[0,1], we obtain
V(t,v(t),η)≤V(t0,v0,η)exp[χ(t−t0)] | (5.15) |
where χ=λM(F2)λ−1M(F1), χ<0.
Next, the estimate (5.15) and condition 2 of Theorem 5.8 imply that
d[v(t),θ0]≤Δ−1ρ1λ1ρM(F1)γ1ρ(d[v0,θ0])exp[χρ(t−t0)], t≥t0, κ∈[0,1]. | (5.16) |
Hence, for
β(⋅)=Δ−1ρ1λ1ρM(F1)γ1ρ(d[v0,θ0]) and λ=−χρ, |
we have an exponential type convergence of an arbitrary solution vκ(t) of (3.5) to the state θ0, which proves the theorem.
We will next establish stability criteria by means of the vector comparison function of type (4.6).
Theorem 5.9. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, and that there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.6) satisfies the following conditions:
1) L(t,v,η) satisfies all conditions of Theorem 4.9;
2) There exist vector functions a,b∈K and constant positive definite (2×2) matrices A1 and A2 such that for the function
V0(t,v,η)=2∑i=1Li(t,v,η) | (5.17) |
the inequalities
aT(d[v,θ0])A1a(d[v,θ0])≤V0(t,v,η)≤bT(d[v,θ0])A2b(d[v,θ0]) | (5.18) |
hold for (t,v,η)∈R+×D(ρ)×R2+.
Then, the stability properties of the zero solution of the vector comparison equation (4.21) imply the corresponding stability properties of the state θ0 of (3.5).
Proof. We will study the equi-asymptotic stability of the steady state θ0 of the regularized system (3.5).
Let 0<ε<ρ and t0∈R+ be given. Suppose that the zero solution of (4.21) is equi-asymptotically stable. Hence, it is stable, and for given λm(A1)¯a(ε)>0 and t0∈R+ there exists δ1=δ1(t0,ε)>0 such that
2∑i=1ωi0<δ1 | (5.19) |
implies that
2∑i=1rMi(t;t0,ω0)<λm(A1)¯a(ε), t≥t0, |
where rM(t;t0,ω0)=(rM1(t;t0,ω0),rM2(t;t0,ω0))T and ¯a∈K exists such that aT(d[v,θ0])a(d[v,θ0])≥¯a(d[v,θ0]) on D(ρ).
We set ω0=V0(t0,v0,η) and choose δ=δ(t0,ε)>0 so that
λM(A2)¯b(δ)<λm(A1)¯a(ε). | (5.20) |
We will prove that if d[ω0,θ0]<δ, then d[v(t;t0,v0),θ0]<ε for all t≥t0 and all κ∈[0,1], where v(t;t0,v0) is an arbitrary solution of (3.5).
If the above assertion is not true, then there exists t1>t0 such that
d[v(t1;t0,v0),θ0]=εandd[v(t;t0,v0),θ0]≤ε<ρ, 0≤t≤t1. |
Since L(t,v,η) satisfies all conditions of Theorem 4.9, we have
L(t,v(t),η)≤rM(t;t0,ω0), t∈[t0,t1], κ∈[0,1]. | (5.21) |
From (5.18), we have
V0(t0,v0,η)≤λM(A2)¯b(d[v0,θ0])<λM(A2)¯b(δ)<δ1 |
and, hence
λm(A1)¯a(ε)≤V0(t1,v(t1),η)≤r0(t1;t0,ω0)<λM(A2)¯b(ε)<λm(A1)¯a(ε), | (5.22) |
where r0(t1;t0,ω0)=2∑i=1rMi(t;t0,ω0).
The contradiction (5.22) proves that the state θ0 of the regularized system (3.5) is equi-stable.
We will next prove that it is attractive. Let ε=ρ and ˆδ0=δ(t0,ρ)>0. We choose 0<σ<ρ and for given λm(A1)¯a(σ) and t0∈R+ choose δ∗1=δ∗1(t0,σ)>0 and τ=τ(t0,σ)>0 so that
2∑i=1ωi0<δ∗1 | (5.23) |
implies that
2∑i=1rMi(t;t0,ω0)<λm(A1)¯a(σ), t≥t0+τ. |
Let ω0=V0(t0,v0,η). Determine δ∗0=δ∗0(t0,σ)>0 so that λM(A2)¯b(δ∗0)<δ∗1. Choose δ0=min(δ∗1,δ∗0) and assume that d[ω0,θ0]<δ0. Hence, d[v(t;t0,v0),θ0]<ρ for all t≥t0 and κ∈[0,1], and therefore, the estimate (5.21) is satisfied for all t≥t0, κ∈[0,1]. Suppose that there exists a sequence {tk}, tk≥t0+τ, tk→+∞ as k→+∞ and σ≤d[v(tk),θ0], where v(t) is an arbitrary solution of (3.5) with initial data v0∈En such that d[v0,θ0]<δ0, and such that the Hukuhara difference u0−w0=v0 exists.
Finally, from (5.18) and (5.23), we have
λm(A1)¯a(σ)≤V0(tk,vκ(tk),η)≤r0(tk,t0,ω0)<λm(A1)¯a(σ). | (5.24) |
The obtained above contradiction (5.24) proves that the stationary state θ0 of (3.5) is attractive and, therefore, quasi-asymptotically stable.
The other stability properties can be proved similarly by linking the dynamic properties of the regularized fuzzy system (3.5) and these of the comparison system (4.21).
Remark 5.10. The established stability criteria show that the idea of using a family of mappings and regularized fuzzy systems of type (3.1) with respect to uncertain parameters greatly benefits their stability analysis. In fact, due to some complications in the study of fuzzy differential systems with uncertain parameters, the proposed results in this direction are very few [20]. Hence, the proposed regularization procedure complements such published accomplishments and, due to the offered advantages is more appropriate for applications. In addition, the modifications of the Lyapunov theory-named matrix-valued Lyapunov functions further extend the advantages of the proposed strategy over the classical Lyapunov function strategies.
Example 5.11. We consider a fuzzy Cohen–Grossberg neural network of Lotka-Volterra type with two interacting species
{du1dt=r1K1u1(t)(K1−u1(t)−e12α12u2(t)),du2dt=r2K2u2(t)(K2−u2(t)−e21α21u1(t)), | (5.25) |
where t≥0; u1(t) and u2(t) are the populations of the two species at time t, respectively, r1 and r2 are intrinsic growth rates; K1 and K2 are the carrying capacities of the environment; e12 and e21 are inter-specific coefficients. All parameters r1, r2, K1, K2 and e12 and e21 are positive numbers. The uncertain parameters are α12 and α21, which can take values from the interval [0,1] and represent the interaction strength between the species.
Introduce the notations
f1(t,u,α)=r1K1u1(t)(K1−u1(t)−e12α12u2(t)), |
f2(t,u,α)=r2K2u2(t)(K2−u2(t)−e21α21u1(t)), |
f(t,u,α)=(f1,f2)T, α=(α12,α21)T, u(t)=(u1(t),u2(t))T. |
Then, the model (5.25) has the following form:
dudt=f(t,u,α), | (5.26) |
where u∈E2 and f∈C(R+×E2×S,E2), S=[0,1]×[0,1].
It is easy to show that for (5.25) there exists an equilibrium uε at
{uε1=K1−K2e12α121−e12e21α12α21,uε2=K2−K1e21α211−e12e21α12α21, | (5.27) |
which is positive for all permissible values of α12 and α21 whenever the carrying capacity ratio K1/K2 satisfies the condition
e12α12<K1K2<1e21α21. |
Now, we consider a regularized system that corresponds to (5.26) and is given by
dvdt=fκ(t,v),v(t0)=v0, | (5.28) |
where fκ∈C(R+×E2,E2) and fm(t,v)=∅ and fκ(t,v)=fM(t,v)κ, κ∈[0,1].
Denote the steady state of (5.28) by θ0. Suppose that there exists a function ˜c(t) such that
(i) d[fκ(t,v),θ0]≤˜c(t)d[v,θ0] for all κ∈[0,1] and (t,v)∈R+×E2;
(ii) ∞∫0˜c(s)ds≤+∞.
If for the corresponding regularized equation (5.8) all conditions H1–H3 are satisfied, then (ⅰ) and (ⅱ) guarantee the uniform stability of its stationary solution θ0∈E2.
In fact, the Lyapunov-type function V(t,v,η)=d[v,θ0] satisfies all conditions of Theorem 5.5. More precisely, V(t,v,η)=ηTU(t,v)η, where the matrix U(t,v) has entries uij(t,v), i,j=1,2 defined as u11(t,v)=u22(t,v)=12d[v,θ0], u12(t,v)=u21(t,v)=0 and η=(1,1)T.
In addition, for any sufficiently small h>0 we have
V(t,v+hfκ(t,v),η)=d[v+hfκ(t,v),θ0] |
≤d[v,θ0]+hd[fκ(t,v),θ0]≤d[v,θ0]+h˜c(t)d[v,θ0]. |
From the definition of the derivative D+V(t,v,η) and (ⅰ), we get
D+V(t,v(t),η)≤˜c(t)d[v,θ0] for any v∈E2. |
Since, condition (ⅱ) is sufficient [18,19] to guarantee the uniform stability of the zero solution of
dm(t)dt=˜c(t)m(t),m(t0)=m0≥0, | (5.29) |
then according to the comparison principle, the state θ0 of the regularized system (5.28) is uniformly stable, too.
In this section, first, under the conditions of Theorem 5.9, we will analyze the stability of the zero solution of the comparison system (4.21) for the case that the vector function G(t,ω) is autonomous. In this case, the comparison system is in the following form:
dωdt=ˉG(ω),ω(t0)=ω0≥0, | (6.1) |
where ˉG∈C(R2+,R2), ˉG=(ˉG1,ˉG2)T, ω=(ω1,ω2)T and the stability problems of the zero solution have effective resolutions under the following assumptions:
(i) The function ˉG is quasimonotonic and nondecreasing with respect to ω on
˜K={ω∈R2: ωi≥0, i=1,2}; |
(ii) There exists a local solution ω(t) of the IVP (6.1) which is uniquely determined by the given initial data;
(iii) There exists a neighborhood D∗ of the state ω=0 such that, for any ω∈¯D∗, we have that ˉG(ω)≠0 for ω≠0 and ˉG(0)=0.
In what follows, uniform asymptotic stability criteria will be established.
Theorem 6.1. Suppose that, for the regularized system (3.5), conditions H1–H3 hold, and that there exist a matrix-valued function U(t,⋅) and a vector η∈R2+ such that the function (4.6) satisfies the following conditions:
1) L(t,v,η) satisfies condition 1 of Theorem 4.9 and condition 2 of Theorem 5.9;
2) L(t,v,η) is such that, for any κ∈[0,1], we have
D+L(t,v,η)≤ˉG(L(t,v,η)), (t,v,η)∈R+×D(ρ)×R2+. | (6.2) |
3) For any δ>0, the system of inequalities
ˉGi(ω1,ω2)<0,i=1,2 |
has a unique solution ¯ω1,¯ω2 such that 0<¯ωi<δ for i=1,2.
Then the state θ0 of (3.5) is uniformly asymptotically stable.
Proof. Under condition 3 of Theorem 6.1, the isolated zero solution of the comparison system (6.1) is uniformly asymptotically stable [18,19]. Further, applying the reasoning from the proof of Theorem 5.9, we complete the proof of Theorem 6.1.
Theorem 6.1 and Corollary 4.10 imply the validity of the following result.
Corollary 6.2. Suppose that, in Theorem 6.1, the function ˉG=ˉG(ω)=Aω and t∈R+, where A is a (2×2) matrix with entries aij≥0 for i≠j.
Then, if the system of inequalities
2∑j=1aij¯ωj<0,i=1,2 |
has a unique solution ¯ω1, ¯ω2 such that 0<¯ωj for all j=1,2, then the state θ0 of the regularized fuzzy system (3.5) is uniformly asymptotically stable
Next, we suppose that
Enm=En1×…×EnmandEni∩Enj=∅ |
for ni≠nj, i,j∈[1,m]. We will represent an autonomous regularized system of the type (3.5) on En1×…×Enm in the following form:
dvi/dt=fiκ(vi)+giκ(v1,…,vm), | (6.3) |
where fiκ∈C(Eni,Eni) and giκ∈C(En1×…×Enm,Eni) for κ∈[0,1], i=1,2,…,m.
We will apply the following two metrics
d0[u,v]=m∑i=1d[ui,vi],whereui,vi∈Eni, | (6.4) |
and
D[u,v]=(d[u1,v1],d[u2,v2],…,d[um,vm])T, | (6.5) |
where D∈Rm+ and u,v∈Enm. Note that the use of the measure (6.4) is related to the following condition
d0[fκ(u),fκ(v)]=m∑i=1d[fiκ(u),fiκ(v)]≤g(d0[u,v])for allκ∈[0,1], | (6.6) |
where g∈C(R+,R+).
The comparison principle for the autonomous regularized system (6.3) is represented as follows.
Theorem 6.3. Suppose that, for the regularized system (6.3), there exists a Lyapunov-type function L(v,η) that satisfies the following conditions:
1) L(v,η)∈C(Enm×R2+,Rm+) and there exists a constant (m×m)−matrix P with real entries such that
||L(v1,η)−L(v2,η)||≤|P|||D[v1,v2]|| |
for v1,v2∈Enm, η∈R2+, where ||.|| is the norm in Rm and |.| is the corresponding matrix norm;
2) There exists a family G(ω), G∈C(Rm+,Rm), such that, for any κ∈[0,1]
D+L(v,η)≤G(L(v,η)), v∈Enm, η∈R2+; |
3) The maximal solution rM(t,t0,ω0) of the comparison equation
dωdt=G(ω),ω(t0)=ω0 | (6.7) |
exists on [t0,∞).
Then, L(v0,η)≤ω0 implies that
L(v(t),η)≤rM(t;t0,ω0), t∈[t0,∞). | (6.8) |
The steps of the proof of Theorem 6.3 are identical to those of the proof of Theorem 2.17 [19].
For the family of equations (6.3), the following result, whose proof is similar to the proof of Theorem 5.9, is valid.
Theorem 6.4. Suppose that for the system (6.3) there exists a vector Lyapunov-type function L(v,η) such that the following holds:
1) L(v,η) satisfies all conditions of Theorem 6.4 for v∈˜D(ρ), where ˜D(ρ)={v∈Enm:d0[v,θ0]<ρ} and η∈R2+;
2) There exist vector functions a,b∈K and constant positive definite (m×m) matrices A1 and A2 such that, for the function
L0(v,η)=m∑i=1Li(v,η) | (6.9) |
for v∈˜Dρ), η∈R2+, we have
aT(d0[v,θ0])A1a(d0[v,θ0])≤L0(v,η)≤bT(d0[v,θ0])A2b(d0[v,θ0]). | (6.10) |
Then the stability properties of the zero solution of the vector comparison equation (6.7) with Gκ(0)=0 imply the corresponding stability properties of the state θ0 of (6.3).
Example 6.5. In this example, we will use functions a∈K such that a→∞ as their variable approaches ∞. Such a class of functions will be denoted as KR. Consider Eq (6.3) under the following assumptions:
1) There exist functions Li(v,η)∈C(Enm×R2+,R+) and ψi1, ψi2∈KR, i=1,2,…,m, such that
ψi1(d0[vi,θ0])≤Li(v,η)≤ψi2(d0[vi,θ0]); |
2) For all i,j=1,2,…,m, there exist constants σi(κ)∈R and aij(κ) such that
(a) D+Li(v,η)≤σi(κ)ψi3(d0[vi,θ0]) with respect to the solutions of the family of equations
dvi/dt=fκ(vi),i=1,2,…,m, κ∈[0,1]; | (6.11) |
(b) D+Li(v,η)≤ψ12i3(d0[vi,θ0])m∑j=1aij(κ)ψ12j(d0[vi,θ0]) on the connection function giκ(v1,…,vm) between subsystems of (6.11) for any κ∈[0,1], i,j=1,2,…,m.
From 1) and 2), for the function V(v,η)=bTL(v,η), b∈Rm+, we have
D+V(v,η)≤ψT3(d0[v,θ0])˜Sψ3(d0[v,θ0]), |
where ψ3=(ψ1213(d0[v1,θ0]),…,ψ12m3(d0[vm,θ0]))T, ˜S=[sij(κ)], i,j=1,2,…,m, κ∈[0,1],
sij(κ)={bi(σi(κ)+aij(κ))fori=j,12(biaij(κ)+bjaji(κ))fori≠j. |
If the matrix ¯M=12(˜ST(κ)+˜S(κ)) is positive definite for all κ∈[0,1], then
D+V(v,η)≤λM(¯M)ψ(d0[v,ˆθ0]), | (6.12) |
where λM(¯M) is the maximal eigenvalue of ¯M for any κ∈[0,1] and the function ψ∈K exists such that ψT3(d0[v,θ0])ψ3(d0[v,θ0])≤ψ(d0[v,θ0]). Condition 1) and (6.12) imply that the stationary state θ0 of (6.3) is uniformly asymptotically stable.
Consider the fuzzy system (3.1) and by means of the regularization process transform it to a regularized system of the following type:
dvdt=fκ(t,v)=gκ(t,v)+hκ(t,v), | (7.1) |
v(t0)=v0, v0∈En2, | (7.2) |
where fκ(t,v) is defined by (3.2) for all κ∈[0,1], gκ, hκ∈C(R+×En2, En2), hκ(t,v)≠0 for v=0 and t∈R+.
For the above fuzzy system (7.1), assume that there exist a unique steady state θ0 and functions ˜f(t) and ˜m(t) that are positive and integrable on any finite interval in R+ such that the following holds:
H4. For any κ∈[0,1] and (t,v)∈R+×En2,
d[gκ(t,v),θ0]≤˜f(t)d[v,θ0]; |
H5. For any κ∈[0,1] and (t,v)∈R+×En2 and k>1
d[hκ(t,v),θ0]≤˜m(t)dk[v,θ0]; |
H6. For all t≥t0, t0∈R+
Φ(t0,t)=(k−1)dk−1[v0,θ0]t∫t0˜m(s)exp[(k−1)s∫t0˜f(τ)dτ]ds<1. |
Now, the goal of our investigations is to obtain boundedness criteria for the family of solutions v(t) of the set of fuzzy differential equations (7.1) for any κ∈[0,1].
Lemma 7.1. Suppose that, for the system (7.1), conditions H4–H6 hold for all t∈[t0,a). Then, for the function V(t,v,η)=d[v,θ0], the estimate
d[v(t),θ0]≤d[v0,θ0]exp(t∫t0˜f(s)ds)(1−Φ(t0,t))−1k−1 | (7.3) |
is satisfied for all t∈[t0,a).
Proof. Without loss of generality, we can consider the function V(t,v,η)=d[v,θ0] for d[v,θ0]≥K∗, where K∗ is sufficiently large. We have that
K1d[v,θ0]≤V(t,v,η)≤K2d[v,θ0] | (7.4) |
for any 0<K1<K2 and all v∈En2.
For the total derivative of the function V(t,v,η) with respect to system (7.1) from H4 and H5, we obtain
D+V(t,v,η)≤˜f(t)d[v,θ0]+˜m(t)dk[v,θ0] | (7.5) |
for any (t,v)∈R+×En2, η=(1,1)T and k>1.
From the above estimate, we get
d[v(t),θ0]≤d[v0,θ0]+t∫t0(˜f(s)d[v(s),θ0]+˜m(s)dk[v(s),θ0])ds, t∈[t0,a). | (7.6) |
Set z(t)=V(t,v(t),η)=d[v(t),θ0]. Then, z(t0)=d[v0,θ0] and the estimate (7.6) has the following form:
z(t)≤z(t0)+t∫t0(˜f(s)z(s)+˜m(s)zk(s))ds=z(t0)+t∫t0(˜f(s)+˜m(s)zk−1(s))z(s)ds, t∈[t0,a). | (7.7) |
We apply the Gronwall-Bellman inequality to the above estimate and get
z(t)≤z(t0)exp(t∫t0(˜f(s)+˜m(s)zk−1(s))ds). | (7.8) |
The estimate (7.8) leads to
zk−1(t)≤zk−1(t0)exp((k−1)t∫t0(˜f(s)+˜m(s)zk−1(s))ds). | (7.9) |
We multiply both sides of (7.9) by the negative expression
−(k−1)˜m(t)exp(−(k−1)t∫t0˜m(s)zk−1(s)ds), |
and we obtain
−(k−1)˜m(t)zk−1(t)exp(−(k−1)t∫t0˜m(s)zk−1(s)ds) |
≥−(k−1)zk−1(t0)˜m(t)exp((k−1)t∫t0˜f(s)ds). |
Hence,
ddt(exp(−(k−1)t∫t0˜m(s)zk−1(s)ds))≥−(k−1)zk−1(t0)˜m(t)exp((k−1)t∫t0˜f(s)ds). | (7.10) |
From (7.10), we obtain
exp(−(k−1)t∫t0˜m(s)zk−1(s)ds)≥1−(k−1)zk−1(t0)t∫t0˜m(s)exp((k−1)s∫t0˜f(τ)dτ)ds. | (7.11) |
The assumption H6 and (7.11) lead to
exp((k−1)t∫t0˜m(s)zk−1(s)ds)≤Φ−1(t,t0)for allt∈[t0,a). |
Considering (7.9) and (7.10), we find that
zk−1(t)≤zk−1(t0)exp((k−1)t∫t0˜f(s)ds)1−(k−1)zk−1(t0)t∫t0˜m(s)exp((k−1)s∫t0˜f(τ)dτ)ds. | (7.12) |
Finally, (7.8) and (7.12) imply (7.3).
We introduce the following boundedness definitions [14,20].
Definition 7.2 The family of solutions v(t)=v(t;t0,v0) of the initial value problem (7.1) and (7.2) is
B1 bounded if there exists a constant r>0 such that, for any t0∈R+ and v0∈En2, we have that d[v(t;t0,v0),θ0]<r for all t≥t0 and all κ∈[0,1], where r may depend on any solution of the set of equations given by (7.1);
B2 equi-bounded if, for any t0∈R+ and δ>0, there exists r=r(t0,δ) such that, for any initial data v0∈En2, d[v0,θ0]<δ implies that d[v(t;t0,v0),θ0]<r for all t≥t0 and all κ∈[0,1];
B3 uniformly bounded if r in B2 does not depend on t0;
B4 quasi-equi-ultimately bounded with a bound ˉr if there exists ˉr>0 and, for any δ0>0, there exists τ=τ(t0,δ)>0 such that d[v0,θ0]<δ0 implies that d[v(t;t0,v0),θ0]<ˉr for all t≥t0+τ and κ∈[0,1];
B5 quasi-uniformly ultimately bounded with a bound ˉr if τ in B4 is independent on t0;
B6 equi-ultimately bounded with a bound ˉr if B2 and B4 hold simultaneously;
B7 uniformly ultimately bounded with a bound ˉr if B3 and B5 hold simultaneously;
B8 equi-stable in the Lagrange sense if B2 and S3 hold simultaneously;
B9 uniformly stable in the Lagrange sense if B3 and S4 hold simultaneously.
Theorem 7.3. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Lemma 7.1 are satisfied and
exp(t∫t0˜f(s)ds)(1−Φ(t,t0))−1k−1<rd[v0,θ0], r>0, t∈[t0,a). | (7.13) |
Then, the family of solutions v(t) is bounded.
Proof. If we suppose that the family of solutions v(t) of (7.1) is unbounded, then, for any r>0 there exists a t1∈[t0,∞) such that
d[v(t),θ0]<r for t∈[t0,t1) and d[v(t1),θ0]=r. |
For the function V(t,v,η)=d[v,θ0], the estimate (7.3) and condition (7.13) imply that d[v(t1),θ0]<r for all κ∈[0,1]. The obtained contradiction proves the assertion of Theorem 7.3.
Next, we will need the following assumption:
(H∗6). For any δ>0, k>1 and d[v0,θ0]<δ, we have
Φ∗(t0,t)=(k−1)δk−1t∫t0˜m(s)exp[(k−1)s∫t0˜f(τ)dτ]ds<1, t∈[t0,a). |
Theorem 7.4. Assume that, for the set of fuzzy equations given by (7.1), the conditions H4–H∗6 hold for all t∈[t0,a), and that, for any δ>0 and t0∈R+ there exists r=r(t0,δ)>0 such that
exp(t∫t0˜f(s)ds)(1−Φ∗(t0,t))−1k−1<r(t0,δ)δ | (7.14) |
for all t∈[t0,a).
Then, the family of solutions v(t) is equi-bounded.
Proof. Analogously to Lemma 7.1, using conditions H4–H∗6, we obtain
d[v(t),θ0]<δexp(t∫t0˜f(s)ds)(1−Φ∗(t0,t))−1k−1, t∈[t0,a). | (7.15) |
From the estimate (7.15) and condition (7.14), we obtain that d[v(t),θ0]<r(t0,δ) for any t∈[t0,a) and κ∈[0,1] whenever d[v0,θ0]<δ. This proves Theorem 7.4.
The proofs of the following boundedness results are similar to the proof of Theorem 7.4.
Theorem 7.5. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorem 7.4 hold, and that, instead of (7.14), for any δ>0 there exists r∗=r∗(δ)>0 such that
exp(t∫t0˜f(s)ds)(1−Φ∗(t0,t))−1k−1<r∗(δ)δ |
for all t∈[t0,a) uniformly on t0∈R+.
Then, the family of solutions v(t) is uniformly bounded.
Theorem 7.6. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorem 7.4 hold, and that, instead of (7.14), for given ˉβ>0 and τ=τ(t0,δ)∈R+ we have
exp(t∫t0˜f(s)ds)(1−Φ∗(t0,t))−1k−1<ˉβδ, t≥t0+τ. |
Then, the family of solutions v(t) is quasi-equi-ultimately bounded.
Theorem 7.7. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorem 7.4 hold, and that, instead of (7.14), for given ˉr>0 and τ∗=τ∗(δ)∈R+ we have
exp(t∫t0˜f(s)ds)(1−Φ∗(t0,t))−1k−1<ˉrδ |
for all t≥t0+τ∗ uniformly on t0∈R+.
Then, the family of solutions v(t) is quasi-uniformly ultimately bounded with a bound ˉr.
The next result follows directly from Theorems 7.4 and 7.6.
Theorem 7.8. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorems 7.4 and 7.6 hold simultaneously.
Then, the family of solutions v(t) is equi-ultimately bounded with a bound ˉβ.
The proof of the next result follows from the proofs of Theorems 7.5 and 7.7.
Theorem 7.9. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorems 7.5 and 7.7 hold simultaneously.
Then, the family of solutions v(t) is uniformly ultimately bounded with a bound ˉr.
Finally, we will establish Lagrange stability results for the steady state θ0 of (7.1).
Theorem 7.10. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorem 7.4 hold, and that, for any t0∈R+ and ξ>0, there exist δ0(t0,ξ)>0 and τ=τ(t0,ξ)∈R+ such that
exp(t∫t0˜f(s)ds)(1−Φ(t0,t))−1k−1<ξδ0(t0,ξ), t≥t0+τ(t0,ξ). | (7.16) |
Then, the family of solutions v(t) is equi-stable in the Lagrange sense.
Proof. Since all conditions of Theorem 7.4 are satisfied, the family of solutions v(t) is equi-bounded.
In addition, (7.3) and (7.16) imply that d[v(t),θ0]<ξ for any t≥t0+τ(t0,ξ) and κ∈[0,1], whenever d[v0,θ0]<δ0(t0,ξ). This proves that the steady state θ0 of (7.1) is quasi-equi-asymptotically stable, which proves Theorem 7.10.
The proof of the last result is similar to the proof of Theorem 7.10.
Theorem 7.11. Assume that, for the set of fuzzy equations given by (7.1), the conditions of Theorem 7.5 hold, and that, for any ξ>0, there exist δ∗(ξ)>0 and τ∗=τ∗(ξ)∈R+ such that, uniformly on t0∈R+,
exp(t∫t0˜f(s)ds)(1−Φ(t0,t))−1k−1<ξδ∗(ξ), t≥t0+τ∗(ξ). |
Then, the family of solutions v(t) is uniformly stable in the Lagrange sense.
Remark 7.12. The proposed boundedness results extend and generalize some existing boundedness and Lagrange stability results for fuzzy systems [38] to the uncertain case. Also, they complement some recently published results [39] in the fuzzy case because of the use of the proposed regularization method.
In this paper, two approaches are proposed for the study of the stability and boundedness of solutions of fuzzy systems of differential equations with uncertain parameters. These approaches are based on the method of matrix-valued Lyapunov-type functions and an integral method based on nonlinear integral inequalities. By applying a new scheme of regularization of fuzzy equations with respect to the inaccuracy parameter [26], numerous new criteria for the stability and boundedness of solutions for regularized equations have been established via the proposed methods. The results obtained can be applied to various fuzzy systems and real-world models in which the effects of some uncertain parameters cannot be neglected. In addition, the proposed methods for the qualitative analysis of fuzzy equations are of decisive importance for many applications, in particular in the theory of motion control. The proposed approaches have significant potential for further generalizations and applications to important classes of fuzzy systems, including systems with delays and impulsive perturbations. An interesting topic for future research is the application of the proposed methods to fuzzy systems with fractional-order dynamics and systems whose dynamics are modeled by fuzzy equations with conformable derivatives of the state vector.
The authors declare that they have not used artificial intelligence tools in the creation of this article.
The authors declare no conflict of interest.
[1] | J. P. LaSalle, S. Lefschetz, Stability by Lyapunov's Second Method with Applications, Academic Press, New York, 1961. Available from: https://www.elsevier.com/books/stability-by-liapunovs-direct-method-with-applications-by-joseph-l-salle-and-solomon-lefschetz/la-salle/978-0-12-437056-2. |
[2] | A. M. Lyapunov, Stability of Motion, Academic Press, New York & London, 1966. Available from: https://www.elsevier.com/books/stability-of-motion/liapunov/978-1-4832-3009-2. |
[3] | G. Leitmann, Deterministic control of uncertain systems via a constructive use of Lyapunov stability theory, in System Modelling and Optimization, Springer, (1990), 38–55. https://doi.org/10.1007/BFb0008354 |
[4] |
M. J. Lacerda, P. Seiler, Stability of uncertain systems using Lyapunov functions with non-monotonic terms, Automatica, 82 (2017), 187–193. https://doi.org/10.1016/j.automatica.2017.04.042 doi: 10.1016/j.automatica.2017.04.042
![]() |
[5] |
G. Stamov, I. M. Stamova, Uncertain impulsive differential systems of fractional order: almost periodic solutions, Int. J. Syst. Sci., 49 (2018), 631–638. https://doi.org/10.1080/00207721.2017.1416428 doi: 10.1080/00207721.2017.1416428
![]() |
[6] |
G. T. Stamov, I. M. Stamova, J. Cao, Uncertain impulsive functional differential systems of fractional order and almost periodicity, J. Franklin Inst., 355 (2018), 5310–5323. https://doi.org/10.1016/j.jfranklin.2018.05.021 doi: 10.1016/j.jfranklin.2018.05.021
![]() |
[7] |
F. Z. Taousser, M. Defoort, M. Djemai, Stability analysis of a class of uncertain switched systems on time scale using Lyapunov functions, Nonlinear Anal. Hybrid Syst., 16 (2015), 13–23. https://doi.org/10.1016/j.nahs.2014.12.001 doi: 10.1016/j.nahs.2014.12.001
![]() |
[8] |
Z. Liu, L. Jia, Cross-validation for the uncertain Chapman-Richards growth model with imprecise observations, Int. J. Uncertainty Fuzziness Knowledge Based Syst., 28 (2020), 769–783. https://doi.org/10.1142/S0218488520500336 doi: 10.1142/S0218488520500336
![]() |
[9] |
P. S. P. Pessim, V. J. S. Leite, M. J. Lacerda, Robust performance for uncertain systems via Lyapunov functions with higher order terms, J. Franklin Inst., 356 (2019), 3072–3089. https://doi.org/10.1016/j.jfranklin.2019.02.004 doi: 10.1016/j.jfranklin.2019.02.004
![]() |
[10] | T. J. Sullivan, Introduction to Uncertainty Quantification, Springer, Cham, 2015. https://doi.org/10.1007/978-3-319-23395-6 |
[11] |
X. Xu, C. Huang, C. Li, G. Zhao, X. Li, C. Ma, Uncertain design optimization of automobile structures: a survey, Electron. Res. Arch., 31 (2023), 1212–1239. https://doi.org/10.3934/era.2023062 doi: 10.3934/era.2023062
![]() |
[12] |
G. W. Wei, Uncertain linguistic hybrid geometric mean operator and its application to group decision making under uncertain linguistic environment, Int. J. Uncertainty Fuzziness Knowledge Based Syst., 17 (2009), 251–267. https://doi.org/10.1142/S021848850900584X doi: 10.1142/S021848850900584X
![]() |
[13] | A. A. Martynyuk, Y. A. Martynyuk-Chernienko, Uncertain Dynamical Systems——Stability and Motion Control, CRC Press, Boca Raton, 2012. https://doi.org/10.1201/b11314 |
[14] | V. Lakshmikantham, S. Leela, A. A. Martynyuk, Stability Analysis of Nonlinear Systems, Birkhauser, Cham, 2015. https://doi.org/10.1007/978-3-319-27200-9 |
[15] | V. Lakshmikantham, V. M. Matrosov, S. Sivasundaram, Vector Lyapunov Functions and Stability Analysis of Nonlinear Systems, Springer Dordrecht, 1991. https://doi.org/10.1007/978-94-015-7939-1 |
[16] |
V. M. Matrosov, Vector Lyapunov function method: theory and applications to complex industrial systems, IFAC Proc. Vol., 30 (1997), 49–62. https://doi.org/10.1016/S1474-6670(17)43346-5 doi: 10.1016/S1474-6670(17)43346-5
![]() |
[17] |
I. M. Stamova, Vector Lyapunov functions for practical stability of nonlinear impulsive functional differential equations, J. Math. Anal. Appl., 325 (2007), 612–623. https://doi.org/10.1016/j.jmaa.2006.02.019 doi: 10.1016/j.jmaa.2006.02.019
![]() |
[18] | A. A. Martynyuk, Stability by Liapunov's Matrix Function Method with Applications, CRC Press, New York, 1998. Available from: https://www.amazon.com/Stability-Liapunovs-Function-Applications-Mathematics/dp/0824701917. |
[19] | A. A. Martynyuk, Qualitative Methods in Nonlinear Dynamics. Novel Approaches to Liapunov's Matrix Functions, Marcel Dekker, Inc., New York, 2002. Available from: https://www.routledge.com/Qualitative-Methods-in-Nonlinear-Dynamics-Novel-Approaches-to-Liapunovs/Martynyuk/p/book/9780367396770. |
[20] | V. Lakshmikantham, R. N. Mohapatra, Theory of Fuzzy Differential Equations and Inclusions, CRC Press, London, 2003. https://doi.org/10.1201/9780203011386 |
[21] |
X. Fan, Z. Wang, A fuzzy Lyapunov function method to stability analysis of fractional-order T–S fuzzy systems, IEEE Trans. Fuzzy Syst., 30 (2022), 2769–2776. https://doi.org/10.1109/TFUZZ.2021.3078289 doi: 10.1109/TFUZZ.2021.3078289
![]() |
[22] |
M. B. Gücen, C. Yakar, Strict stability of fuzzy differential equations by Lyapunov functions, Int. J. Inf. Control Comput. Sci., 11 (2018), 1267–1277. https://doi.org/10.5281/zenodo.1316718 doi: 10.5281/zenodo.1316718
![]() |
[23] |
V. Lakshmikantham, S. Leela, Stability theory of fuzzy differential equations via differential inequalities, Math. Inequal. Appl., 2 (1999), 551–559. https://doi.org/10.7153/mia-02-46 doi: 10.7153/mia-02-46
![]() |
[24] |
S. Song, C. Wu, E. S. Lee, Asymptotic equilibrium and stability of fuzzy differential equations, Comput. Math. Appl., 49 (2005), 1267–1277. https://doi.org/10.1016/j.camwa.2004.03.016 doi: 10.1016/j.camwa.2004.03.016
![]() |
[25] |
Z. P. Yang, W. J. Ren, Existence and stability results for quaternion fuzzy fractional differential equations in the sense of Hilfer, J. Intell. Fuzzy Syst., 34 (2018), 167–175. https://doi.org/10.3233/JIFS-171042 doi: 10.3233/JIFS-171042
![]() |
[26] |
A. Martynyuk, G. Stamov, I. Stamova, Y. Martynyuk-Chernienko, Regularization scheme for uncertain fuzzy differential equations: analysis of solutions, Electron. Res. Arch., 31 (2023), 3832–3847. https://doi.org/10.3934/era.2023195 doi: 10.3934/era.2023195
![]() |
[27] | P. Diamond, P. Kloeden, Metric Spaces of Fuzzy Sets: Theory and Applications, World Scientific, Singapore, 1994. Available from: https://www.worldscientific.com/worldscibooks/10.1142/2326#t = aboutBook. |
[28] | C. V. Negoita, D. A. Ralescu, Applications of Fuzzy Sets to System Analysis, Springer, Basel, 1975. Available from: https://link.springer.com/book/10.1007/978-3-0348-5921-9. |
[29] | H. J. Zimmermann, Fuzzy Set Theory——and Its Applications, Springer, New York, 2001. Available from: https://link.springer.com/book/10.1007/978-94-010-0646-0. |
[30] | K. Deimling, Multivalued Differential Equations, Walter de Gruyter, New York, 1992. https://doi.org/10.1515/9783110874228 |
[31] |
M. L. Puri, D. A. Ralescu, Differentials of fuzzy functions, J. Math. Anal. Appl., 91 (1983), 552–558. https://doi.org/10.1016/0022-247X(83)90169-5 doi: 10.1016/0022-247X(83)90169-5
![]() |
[32] |
L. A. Zadeh, Fuzzy sets, Inf. Control, 8 (1965), 338–353. https://doi.org/10.1016/S0019-9958(65)90241-X doi: 10.1016/S0019-9958(65)90241-X
![]() |
[33] |
J. J. Buckley, T. Feuring, Fuzzy differential equations, Fuzzy Sets Syst., 110 (2000), 43–54. https://doi.org/10.1016/S0165-0114(98)00141-9 doi: 10.1016/S0165-0114(98)00141-9
![]() |
[34] |
O. Kaleva, Fuzzy differential equations, Fuzzy Sets Syst., 24 (1987), 301–317. https://doi.org/10.1016/0165-0114(87)90029-7 doi: 10.1016/0165-0114(87)90029-7
![]() |
[35] |
O. Kaleva, The Peano theorem for fuzzy differential equations revisited, Fuzzy Sets Syst., 98 (1998), 147–148. https://doi.org/10.1016/S0165-0114(97)00415-6 doi: 10.1016/S0165-0114(97)00415-6
![]() |
[36] |
D. Vorobiev, S. Seikkala, Towards the theory of fuzzy differential equations, Fuzzy Sets Syst., 125 (2002), 231–237. https://doi.org/10.1016/S0165-0114(00)00131-7 doi: 10.1016/S0165-0114(00)00131-7
![]() |
[37] |
M. Mazandarani, L. Xiu, A review on fuzzy differential equations, IEEE Access, 9 (2021), 62195–62211. https://doi.org/10.1109/ACCESS.2021.3074245 doi: 10.1109/ACCESS.2021.3074245
![]() |
[38] |
C. Yakar, M. Çiçek, M. B. Gücen, Practical stability, boundedness criteria and Lagrange stability of fuzzy differential systems, Comput. Math. Appl., 64 (2012), 2118–2127. https://doi.org/10.1016/j.camwa.2012.04.008 doi: 10.1016/j.camwa.2012.04.008
![]() |
[39] |
A. Martynyuk, I. Stamova, Y. A. Martynyuk-Chernienko, On the boundedness and Lagrange stability of fractional-like neural network-based quasilinear systems, Eur. Phys. J. Spec. Top., 231 (2022), 1789–1799. https://doi.org/10.1140/epjs/s11734-022-00447-3 doi: 10.1140/epjs/s11734-022-00447-3
![]() |