Successful identification procedures are undoubtedly important for accurate model description and the consequent implementation of control strategies. Linear Parameter Varying (LPV) models are nowadays standard for control design purposes and powerful identification techniques accordingly available. Anyhow, recent advances have brought to focus the class of Nonlinear Parameter Varying (NLPV) models, which keep some nonlinearities embedded to the formulation. Identification tools for this latter class are still not available. Therefore, this paper proposes a novel method for the robust identification of stochastic NLPV systems, considering that the nonlinear parameter part is a priori known and obeys a Lipschitz condition. The method is based on a modified extended Masreliez-Martin filter and yields the joint estimation of both NLPV systems states and model parameters. The method manages the stochasticity of the system by considering the presence of measurement outliers with non-Gaussian distributions. Results considering real data from a vehicle suspension system are presented in order to demonstrate the consistency of the proposed method.
Citation: Marcelo Menezes Morato, Vladimir Stojanovic. A robust identification method for stochastic nonlinear parameter varying systems[J]. Mathematical Modelling and Control, 2021, 1(1): 35-51. doi: 10.3934/mmc.2021004
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Successful identification procedures are undoubtedly important for accurate model description and the consequent implementation of control strategies. Linear Parameter Varying (LPV) models are nowadays standard for control design purposes and powerful identification techniques accordingly available. Anyhow, recent advances have brought to focus the class of Nonlinear Parameter Varying (NLPV) models, which keep some nonlinearities embedded to the formulation. Identification tools for this latter class are still not available. Therefore, this paper proposes a novel method for the robust identification of stochastic NLPV systems, considering that the nonlinear parameter part is a priori known and obeys a Lipschitz condition. The method is based on a modified extended Masreliez-Martin filter and yields the joint estimation of both NLPV systems states and model parameters. The method manages the stochasticity of the system by considering the presence of measurement outliers with non-Gaussian distributions. Results considering real data from a vehicle suspension system are presented in order to demonstrate the consistency of the proposed method.
The theme of fractional calculus (FC) has appeared as a broad and interesting research point due to its broad applications in science and engineering. FC is now greatly evolved and embraces a wide scope of interesting findings. To obtain detailed information on applications and recent results about this topic, we refer to [1,2,3,4,5] and the references therein.
Some researchers in the field of FC have realized that innovation for new FDs with many non-singular or singular kernels is very necessary to address the need for more realistic modeling problems in different fields of engineering and science. For instance, we refer to works of Caputo and Fabrizio [6], Losada and Nieto [7] and Atangana-Baleanu [8]. The class of FDs and fractional integrals (FIs) concerning functions is a considerable branch of FC. This class of operators with analytic kernels is a new evolution proposed in [1,9,10]. Every one of these operators is appropriate broader to cover various kinds of FC and catch diversified behaviors in fractional models. Joining the previous ideas yields another, significantly wide, which is a class of function-dependent-kernel fractional derivatives. This covers both of the two preceding aforesaid classes see [11,12].
In another context, the Langevin equations (LEs) were formulated by Paul Langevin in 1908 to describe the development of physical phenomena in fluctuating environments [13]. After that, diverse generalizations of the Langevin equation have been deliberated by many scholars we mention here some works [14,15,16]. Recently, many researchers have investigated sufficient conditions of the qualitative properties of solutions for the nonlinear fractional LEs involving various types of fractional derivatives (FDs) and by using different types of methods such as standard fixed point theorems (FPTs), Leray-Schauder theory, variational methods, etc., e.g. [17,18,19,20,21,22,23,24]. Some recent results on the qualitative properties of solutions for fractional LEs with the generalized Caputo FDs can be found in [25,26,27,28,29,30], e.g., Ahmad et al. [25] established the existence results for a nonlinear LE involving a generalized Liouville-Caputo-type
{ρcDα1a+(ρcDα2a++λ)z(ς)=F(ς,z(ς)),ς∈[a,T], λ∈R,z(a)=0,z(η)=0, z(T)=μ ρIδa+z(ξ), a<η<ξ<T. | (1.1) |
Seemab et al. [26] investigated the existence and UHR stability results for a nonlinear implicit LE involving a ϑ -Caputo FD
{cDα1,ϑa+(cDα2,ϑa++λ)z(ς)=F(ς,z(ς),cDα1,ϑa+z(ς)),ς∈(a,T), λ>0,z(a)=0,z(η)=0, z(T)=μ Iδ;ϑa+z(ξ), 0≤a<η<ξ<T<∞. | (1.2) |
The Hyers-Ulam (U-H) stability and existence for various types of generalized FDEs are established in the papers [31,32,33,34,35,36,37,38,39,40,41,42,43].
Motivated by the above works and inspired by novel developments in ϑ -FC, in the reported research, we investigate the existence, uniqueness, and U-H-type stability of the solutions for the nonlinear fractional Langevin differential equation (for short FLDE) described by
{Dα2;ϑa+(Dα1;ϑa++λ)z(ς)=F(ς,z(ς)),ς∈J=[a,b],z(a)=0,z′(a)=0,z′′(a)=0,Dα1;ϑa+z(a)=Iδ;ϑa+z(ξ),Dα1;ϑa+z(b)+κz(b)=0, | (1.3) |
where Dε;ϑa+ denote the ϑ-Caputo FD of order ε∈{α1,α2} such that α1∈(2,3], α2∈(1,2], ξ∈(a,b), δ>0, Iα1;ϑa+ is the ϑ-fractional integral of the Riemann-Liouville (RL) type, F:J×R→R is a continuous function, and λ,κ ∈R, ξ∈(a,b).
The considered problem in this work is more general, in other words, when we take certain values of function ϑ, the problem (1.3) is reduced to many problems in the frame of classical fractional operators. Also, the gained results here are novel contributes and an extension of the evolution of FDEs that involving a generalized Caputo operator, especially, the study of stability analysis of Ulam-Hyers type of fractional Langevin equations is a qualitative addition to this work. Besides, analysis of the results was restricted to a minimum of assumptions.
Here is a brief outline of the paper. Section 2 provides the definitions and preliminary results required to prove our main findings. In Section 3, we establish the existence, uniqueness, and stability in the sense of Ulam for the system (1.3). In Section 5, we give some related examples to light the gained results.
We start this part by giving some basic definitions and results required for fractional analysis.
Consider the space of real and continuous functions U=C(J,R) space with the norm
‖z‖∞=sup{|z(ς)|:ς∈J}. |
Let ϑ∈C1=C1(J,R) be an increasing differentiable function such that ϑ′(ς)≠0, for all ς∈J.
Now, we start by defining ϑ-fractionals operators as follows:
Definition 2.1. [1] The ϑ-RL fractional integral of order α1>0 for an integrable function ω:J⟶R is given by
Iα1;ϑa+ω(ς)=1Γ(α1)∫ςaϑ′(s)(ϑ(ς)−ϑ(s))α1−1ω(s)ds. | (2.1) |
Definition 2.2. [1] Let α1∈(n−1,n), n∈N, ω:J→R is an integrable function, and ϑ∈Cn(J,R), the ϑ-RL FD of a function ω of order α1 is given by
Dα1;ϑa+ω(ς)=(Dςϑ′(ς))n In−α1;ϑa+ω(ς), |
where n=[α1]+1 and Dς=ddt.
Definition 2.3. [9] For α1∈(n−1,n), and ω,ϑ∈Cn(J,R), the ϑ-Caputo FD of a function ω of order α1 is given by
cDα1;ϑa+ω(ς)= In−α1;ϑa+ω[n]ϑ(ς), |
where n=[α1]+1 for α1∉N, n=α1 for α1∈N, and ω[n]ϑ(ς)=(Dςϑ′(ς))nω(ς).
From the above definition, we can express ϑ-Caputo FD by formula
cDα1;ϑa+ω(ς)={∫ςaϑ′(s)(ϑ(ς)−ϑ(s))n−α1−1Γ(n−α1)ω[n]ϑ(s)ds,ifα1∉N,ω[n]ϑ(ς),ifα1∈N. | (2.2) |
Also, the ϑ-Caputo FD of order α1 of ω is defined as
cDα1;ϑa+ω(ς)=Dα1;ϑa+[ω(ς)−n−1∑k=0ω[k]ϑ(a)k!(ϑ(ς)−ϑ(a))k]. |
For more details see [9,Theorem 3].
Lemma 2.4. [1] For α1,α2>0, and ω∈C(J,R), we have
Iα1;ϑa+Iα2;ϑa+ω(ς)=Iα1+α2;ϑa+ω(ς),a.e.ς∈J. |
Lemma 2.5. [44] Let α1>0.
If ω∈C(J,R), then
cDα1;ϑa+Iα1;ϑa+ω(ς)=ω(ς),ς∈J, |
and if ω∈Cn−1(J,R), then
Iα1;ϑa+cDα1;ϑa+ω(ς)=ω(ς)−n−1∑k=0ω[k]ϑ(a)k![ϑ(ς)−ϑ(a)]k,ς∈J. |
for all ς∈J. Moreover, if m∈N be an integer and ω∈Cn+m(J,R) a function. Then, the following holds:
(1ϑ′(ς)ddt)m⋅Dα1;ϕa+ω(ς)= cDa+m;ϕa+ω(ς)+m−1∑k=0(ϑ(ς)−ϑ(a))k+n−^α1−mΓ(k+n−α1−m+1)ω[k+n]ϑ(a) | (2.3) |
Observe that from Eq (2.3), if ω[k]ϑ(a)=0, for all k=n,n+1,…,n+m−1 we can get the following relation
z[m]ϑ⋅Da,ϑa+z(ς)= cDα1+m;ϑa+z(ς),ς∈J |
Lemma 2.6. [1,9] For ς>a,α1≥0, α2>0, we have
● Iα1;ϑa+(ϑ(ς)−ϑ(a))α2−1=Γ(α2)Γ(α2+α1)(ϑ(ς)−ϑ(a))α2+α1−1,
● cDα1;ϑa+(ϑ(ς)−ϑ(a))α2−1=Γ(α2)Γ(α2−α1)(ϑ(ς)−ϑ(a))α2−α1−1,
● cDα1;ϑa+(ϑ(ς)−ϑ(a))k=0,∀k∈{0,…,n−1},n∈N.
Theorem 2.7. (Banach's FPT [45]). Let (R,d) be a nonempty complete metric space with a contraction mapping G:R→R i.e., d(Gz,Gϰ)≤Ld(z,ϰ) for all z,ϰ∈R, where L∈(0,1) is a constant. Then G possesses a unique fixed point.
Theorem 2.8. (Kransnoselskii's FPT [46]). Let E be a Banach space. Let S is a nonempty convex, closed and bounded subset of E and let A1,A2 be mapping from S to E such that:
(i) A1z+A2ϰ∈S whenever z,ϰ∈S
(ii) A1 is continuous and compact;
(iii) A2 is a contraction.
Then there exists z∈S such that z=A1z+A2z.
This portion interests in the existence, uniqueness, and Ulam stability of solutions to the suggested problem (1.3).
The next auxiliary lemma, which attentions the linear term of a problem (1.3), plays a central role in the afterward findings.
Lemma 3.1. Let α1∈(2,3], α2∈(1,2]. Then the linear BVP
{Dα2;ϑa+(Dα1;ϑ+λ)z(ς)=σ(ς),ς∈J=[a,b],z(a)=0,z′(a)=0,z′′(a)=0,Dα1;ϑa+z(a)=Iδ;ϑa+z(γ),Dα1;ϑa+z(b)+κz(b)=0, | (3.1) |
has a unique solution defined by
z(ς)=Iα1+α2;ϑa+σ(ς)−λIα1;ϑa+z(ς)+μ(ς)Iδ;ϑa+σ(ξ)+ν(ς){λ(κ−λ)Iα1;ϑa+z(b)−(κ−λ)Iα1+α2;ϑa+σ(b)−Iα2;ϑa+σ(b)−ϖIδ;ϑa+z(ξ)}, | (3.2) |
where
μ(ς)=(ϑ(ς)−ϑ(a))α1Γ(α1+1), | (3.3) |
and
ν(ς)=(ϑ(ς)−ϑ(a))α1+1(ϑ(b)−ϑ(a))Γ(α1+2)+(κ−λ), | (3.4) |
with
ϖ=(1+(κ−λ)Γ(α1+1)), | (3.5) |
Proof. Applying the RL operator Iα2;ϑa+ to (3.1) it follows from Lemma 2.5 that
(Dα1a++λ)z(ς)=c0+c1(ϑ(ς)−ϑ(a))+Iα2;ϑa+σ(ς),ς∈(a,b]. | (3.6) |
Again, we apply the RL operator Iα1;ϑa+ and use the results of Lemma 2.5 to get
z(ς)=Iα1+α2;ϑa+σ(ς)−λIα1a+z(ς)+c0(ϑ(ς)−ϑ(a))α1+1Γ(α1+2)+c1(ϑ(ς)−ϑ(a))α1Γ(α1+1)+c2(ϑ(ς)−ϑ(a))2+c3(ϑ(ς)−ϑ(a))+c4, | (3.7) |
where c0,c1,c2,c3,c4∈R. By utilizing the boundary conditions in (3.1) and (3.7), we obtain c2=0,c3=0,c4=0.
Hence,
z(ς)=Iα1+α2;ϑa+σ(ς)−λIα1a+z(ς)+c0(ϑ(ς)−ϑ(a))α1+1Γ(α1+2)+c1(ϑ(ς)−ϑ(a))α1Γ(α1+1), | (3.8) |
Now, by using the conditions Dα1;ϑa+z(a)=Iδ;ϑa+z(γ) and Dα1;ϑa+z(b)+κz(b)=0, we get
c1=Iδ;ϑa+z(ξ), | (3.9) |
c0=((ϑ(ς)−ϑ(a))α1+1(ϑ(b)−ϑ(a))Γ(α1+2)+(κ−λ))×{λ(κ−λ)Iα1;ϑa+z(b)−(κ−λ)Iα1+α2;ϑa+σ(b)−Iα2;ϑa+σ(b)−(1+(κ−λ)Γ(α1+1))Iδ;ϑa+z(ξ)}. | (3.10) |
Substituting c0 and c1 in (3.8), we finish with (3.2).
The reverse direction can be shown easily with the help of results in Lemmas 2.5 and 2.6, i.e. Eq (3.2) solves problem (3.1). This ends the proof.
Now, we shall need to the following lemma:
Lemma 3.2. The functions μ and ν are continuous functions on J and satisfy the following properties:
(1) μ∗=max0≤ς≤b|μ(ς)|,
(2) ν∗=max0<ς<b|ν(ς)|,
where μ and ν are defined by Lemma 3.1.
Here, we give the following hypotheses:
(H1) The function F:J×R→R is continuous.
(H2) There exists a constant L>0 such that
|F(ς,z)−F(ς,ϰ)|≤L|z−ϰ|,ς∈J,z,ϰ∈R. |
(H3) There exist positive functions h(ς)∈C(J,R+) with bounds ‖h‖ such that
|F(ς,z(ς))|≤h(ς), for all (ς,z)∈J×R. |
For simplicity, we denote
M:=supς∈[a,b]|F(ς,0)|. |
Δ:={(L(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)(1+ν∗|κ−λ|)+|λ|(1+ν∗|κ−λ|)(ϑ(b)−ϑ(a))α1Γ(α1+1))+(Lν∗(ϑ(b)−ϑ(a))α2Γ(α2+1)+(μ∗+ν∗|ϖ|)(ϑ(ξ)−ϑ(a))δΓ(δ+1))}, | (3.11) |
Gχϑ(ς,s)=ϑ′(s)(ϑ(ς)−ϑ(s))χ−1Γ(χ),χ>0. | (3.12) |
As a result of Lemma 3.1, we have the subsequent lemma:
Lemma 3.3. Suppose that F:J×R→R is continuous. A function z(ς) solves (1.3) if and only if it is a fixed-point of the operator G:U→U defined by
Gz(ς)=∫ςaGα1+α2ϑ(ς,s)F(s,z(s))ds+λ∫ςaGα1ϑ(ς,s)z(s)ds+μ(ς)∫ξaGδϑ(ξ,s)F(s,z(s))ds+ν(ς){λ(κ−λ)∫baGα1ϑ(b,s)z(s)ds−(κ−λ)∫baGα1+α2ϑ(b,s)F(s,z(s))ds−∫baGα2ϑ(b,s)F(s,z(s))ds−ϖ∫ξaGδϑ(ξ,s)z(s)ds}. | (3.13) |
Now, we are willing to give our first result which based on Theorem 2.7.
Theorem 3.4. Suppose that (H1) and (H2) hold. If Δ<1, where Δ is given by (3.11), then there exists a unique solution for (1.3) on the interval J.
Proof. Thanks to Lemma 3.1, we consider the operator G:U→U defined by (3.13). Thus, G is well defined as F is a continuous. Then the fixed point of G coincides with the solution of FLDE (1.3). Next, the Theorem 2.7 will be used to prove that G has a fixed point. For this end, we show that G is a contraction.
Let BR={z∈U:‖z‖≤R}, where R>MΛ11−LΛ1−Λ2. Since
|F(s,z(s)|=|F(s,z(s))−F(s,0)+F(s,0)|≤|F(s,z(s))−F(s,0)|+|F(s,0)|≤(L|z(s)|+|F(s,0)|)≤LR+M |
we obtain
|Gz(ς)|=∫ςaGα1+α2ϑ(ς,s)|F(s,z(s))|ds+|λ|∫ςaGα1ϑ(ς,s)|z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|z(s)|ds+(κ−λ)∫baGα1+α2ϑ(b,s)|F(s,z(s))|ds+∫baGα2ϑ(b,s)|F(s,z(s))|ds+ϖ∫ξaGδϑ(ξ,s)|z(s)|ds}≤LR+M{∫ςaGα1+α2ϑ(ς,s)|F(s,z(s))|ds+ν(ς){|κ−λ|∫baGα1+α2ϑ(b,s)|F(s,z(s))|ds+ν∗∫baGα2ϑ(b,s)|F(s,z(s))|ds}+R{|λ|∫ςaGα1ϑ(ς,s)|z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|z(s)|ds+ϖ∫ξaGδϑ(ξ,s)|z(s)|ds}}≤LR+M{(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)(1+ν∗|κ−λ|)+ν∗(ϑ(b)−ϑ(a))α2Γ(α2+1)}+R{|λ|(1+ν∗|κ−λ|)(ϑ(b)−ϑ(a))α1Γ(α1+1)+(μ∗+ν∗|ϖ|)(ϑ(ξ)−ϑ(a))δΓ(δ+1)}≤(LR+M)Λ1+Λ2R≤R. | (3.14) |
which implies that ‖Gz‖≤R, i.e.,
GBR⊆BR. |
Now, let z,ϰ∈U. Then, for every ς∈J, using (H2), we can get
|Gϰ(ς)−Gz(ς)|≤∫ςaGα1+α2ϑ(ς,s)|F(s,ϰ(s))−F(s,z(s))|ds+|λ|∫ςaGα1ϑ(ς,s)|ϰ(s)−z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|ϰ(s)−z(s)|ds+|κ−λ|∫baGα1+α2ϑ(b,s)|F(s,ϰ(s))−F(s,z(s))|ds+∫baGα2ϑ(b,s)|F(s,ϰ(s))−F(s,z(s))|ds+ϖ∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds}≤∫ςaLGa+α2ϑ(ς,s)|ϰ(s)−z(s)|ds+|λ|∫ςaGα1ϑ(ς,s)|ϰ(s)−z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|ϰ(s)−z(s)|ds+(κ−λ)∫baGα1+α2ϑ(b,s)L|ϰ(s)−z(s)|ds+∫baGα2ϑ(b,s)L|ϰ(s)−z(s)|ds+ϖ∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds}=∫ςa(LGα1+α2ϑ(ς,s)+|λ|Gα1ϑ(ς,s))|ϰ(s)−z(s)|ds+(μ∗+ν∗|ϖ|)∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds+ν∗∫ba(|κ−λ|(λGα1ϑ(b,s)+LGα1+α2ϑ(ς,s))+LGα2ϑ(b,s))|ϰ(s)−z(s)|ds≤‖ϰ−z‖∞{∫ςa(LGα1+α2ϑ(ς,s)+|λ|Gα1ϑ(ς,s))ds+(μ∗+ν∗|ϖ|)∫ξaGδϑ(ξ,s)ds+ν∗∫ba(|κ−λ|(λGα1ϑ(b,s)+LGα1+α2ϑ(ς,s))+LGα2ϑ(b,s))ds} | (3.15) |
Also note that
∫ςaGχϑ(ς,s)ds≤(ϑ(b)−ϑ(a))χΓ(χ+1),χ>0. |
Using the above arguments, we get
‖Gϰ−Gz‖∞≤{(L(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)(1+ν∗|κ−λ|)+|λ|(1+ν∗|κ−λ|)(ϑ(b)−ϑ(a))α1Γ(α1+1))+(Lν∗(ϑ(b)−ϑ(a))α2Γ(α2+1)+(μ∗+ν∗|ϖ|)(ϑ(ξ)−ϑ(a))δΓ(δ+1))}‖ϰ−z‖∞=Δ‖ϰ−z‖∞. |
As Δ<1, we derive that G is a contraction. Hence, by Theorem 2.7, G has a unique fixed point which is a unique solution of FLDE (1.3). This ends the proof.
Now, we apply the Theorem 2.8 to obtain the existence result.
Theorem 3.5. Let us assume (H1)–(H3) hold. Then FLDE (1.3) has at least one solution on J if Λ3<1, where it is supposed that
Λ3:={(L(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)(ν∗|κ−λ|)+|λ|(ν∗|κ−λ|)(ϑ(b)−ϑ(a))α1Γ(α1+1))+(Lν∗(ϑ(b)−ϑ(a))α2Γ(α2+1)+(μ∗+ν∗|ϖ|)(ϑ(ξ)−ϑ(a))δΓ(δ+1))}. |
Proof. By the assumption (H3), we can fix
ρ≥λ1‖h‖(1−λ2), |
where Bρ={z∈U:‖z‖≤ρ}. Let us split the operator G:U→U defined by (3.13) as G=G1+G2, where G1 and G2 are given by
G1z(ς)=∫ςaGα1+α2ϑ(ς,s)F(s,z(s))ds+λ∫ςaGα1ϑ(ς,s)z(s)ds, | (3.16) |
and
G2z(ς)=μ(ς)∫ξaGδϑ(ξ,s)F(s,z(s))ds+ν(ς){λ(κ−λ)∫baGα1ϑ(b,s)z(s)ds−(κ−λ)∫baGα1+α2ϑ(b,s)F(s,z(s))ds−∫baGα2ϑ(b,s)F(s,z(s))ds−ϖ∫ξaGδϑ(ξ,s)z(s)ds}. | (3.17) |
The proof will be split into numerous steps:
Step 1: G1(z)+G2(z)∈Bρ.
‖G1z+G2z1‖=supς∈J|G1z(ς)+G2z1(ς)|≤∫ςaGα1+α2ϑ(ς,s)|F(s,z(s))|ds+|λ|∫ςaGα1ϑ(ς,s)|z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|z(s)|ds+|κ−λ|∫baGα1+α2ϑ(b,s)|F(s,z(s))|ds+∫baGα2ϑ(b,s)|F(s,z(s))|ds+ϖ∫ξaGδϑ(ξ,s)|z(s)|ds} | (3.18) |
≤‖h‖{∫ςaGα1+α2ϑ(ς,s)|F(s,z(s))|ds+ν(ς){|κ−λ|∫baGα1+α2ϑ(b,s)|F(s,z(s))|ds+ν∗∫baGα2ϑ(b,s)|F(s,z(s))|ds}+ρ{|λ|∫ςaGα1ϑ(ς,s)|z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|z(s)|ds+ϖ∫ξaGδϑ(ξ,s)|z(s)|ds}}≤‖h‖{(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)(1+ν∗|κ−λ|)+ν∗(ϑ(b)−ϑ(a))α2Γ(α2+1)}+ρ{|λ|(1+ν∗|κ−λ|)(ϑ(b)−ϑ(a))α1Γ(α1+1)+(μ∗+ν∗|ϖ|)(ϑ(ξ)−ϑ(a))δΓ(δ+1)}≤‖h‖Λ1+Λ2ρ≤ρ. | (3.19) |
Hence
‖G1(z)+G2(z1)‖≤ρ, |
which shows that G1z+G2z1∈Bρ.
Step 2: G2 is a contraction map on Bρ.
Due to the contractility of G as in Theorem 3.4, then G2 is a contraction map too.
Step 3: G1 is completely continuous on Bρ.
From the continuity of F(⋅,z(⋅)), it follows that G1 is continuous.
Since
‖G1z‖=supς∈J|G1z(ς)|≤∫ςaGα1+α2ϑ(ς,s)|F(s,z(s))|ds+|λ|∫ςaGα1ϑ(ς,s)|z(s)|ds≤‖h‖(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)+|λ|(ϑ(b)−ϑ(a))α1Γ(α1+1)ρ:=N, z∈Bρ, |
we get ‖G1z‖≤N which emphasize that G1 uniformly bounded on Bρ.
Finally, we prove the compactness of G1.
For z∈Bρ and ς∈J, we can estimate the operator derivative as follows:
|(G1z)(1)ϑ(ς)|≤∫ςaGα1+α2−1ϑ(ς,s)|F(s,z(s))|ds+|λ|∫ςaGα1−1ϑ(ς,s)|z(s)|ds≤‖h‖(ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)+|λ|(ϑ(b)−ϑ(a))α1Γ(α1+1)ρ:=ℓ, |
where we used the fact
Dkϑ Iα1,ϑa+=Iα1−k,ϑa+, ω(k)ϑ(ς)=(1ϑ′(ς)ddς)kω(ς) for k=0,1,...,n−1. |
Hence, for each ς1,ς2∈J with a<ς1<ς2<b and for z∈Bρ, we get
|(G1z)(ς2)−(G1z)(ς1)|=∫ς2ς1|(G1z)′(s)|ds≤ℓ(ς2−ς1), |
which as (ς2−ς1) tends to zero independent of z. So, G1 is equicontinuous. In light of the foregoing arguments along with Arzela–Ascoli theorem, we derive that G1 is compact on Bρ. Thus, the hypotheses of Theorem 2.8 holds, so there exists at least one solution of (1.3) on J.
In the current section, we are interested in studying Ulam-Hyers (U-H) and the generalized Ulam-Hyers stability types of the problem (1.3).
Let ε>0. We consider the next inequality:
|Dα2;ϑa+(Da;ϑa+−λ)˜z(ς)−F(ς,˜z(ς))|≤ε,ς∈J. | (4.1) |
Definition 4.1. FLDE (1.3) is stable in the frame of U-H type if there exists cF∈R+ such that for every ε>0 and for each solution ˜z∈U of the inequality (4.1) there exists a solution z∈U of (1.3) with
|˜z(ς)−z(ς)|≤εcF,ς∈J. |
Definition 4.2. FLDE (1.3) has the generalized U-H stability if there exists CF: C(R+,R+) along with CF(0)=0 such that for every ε>0 and for each solution ˜z∈U of the inequality (4.1), a solution z∈C(J,R) of (1.3) exists uniquely for which
|˜z(ς)−z(ς)|≤CF(ε),ς∈J. |
Remark 4.3. A function ˜z∈U is a solution of the inequality (4.1) if and only if there exists a function ϱ∈U (which depends on solution ˜z) such that
1.|ϱ(ς)|≤ε,ς∈J.
2.Dα2;ϑa+(Da,ϑa+−λ)˜z(ς)=F(ς,˜z(ς))+ϱ(ς),ς∈J.
Theorem 4.4. Let Δ<1, (H1) and (H2) hold. Then the FLDE (1.3) is U-H stable on J and consequently generalized U-H stable.
Proof. For ε>0 and ˜z∈C(J,R) be a function which fulfills the inequality (4.1). Let z∈U the unique solution of
{Dα2;ϑa+(Dα1;ϑ+λ)z(ς)=F(ς,z(ς)),ς∈J=[a,b],z(a)=0,z′(a)=0,z′′(a)=0,Dα1;ϑa+z(a)=Iδ;ϑa+z(γ),Dα1;ϑa+z(b)+κz(b)=0. | (4.2) |
By Lemma 3.1, we have
z(ς)=∫ςaGα1+α2ϑ(ς,s)F(s,z(s))ds+λ∫ςaGα1ϑ(ς,s)z(s)ds+μ(ς)∫ξaGδϑ(ξ,s)F(s,z(s))ds+ν(ς){λ(κ−λ)∫baGα1ϑ(b,s)z(s)ds−(κ−λ)∫baGα1+α2ϑ(b,s)F(s,z(s))ds−∫baGα2ϑ(b,s)F(s,z(s))ds−ϖ∫ξaGδϑ(ξ,s)z(s)ds}. | (4.3) |
Since we have assumed that ˜z is a solution of (4.1), hence by Remark 4.3
{Dα2;ϑa+(Dα1;ϑa++λ)˜z(ς)=F(ς,˜z(ς))+ϱ(ς),ς∈J=[0,b],z(a)=0,z′(a)=0,z′′(a)=0,Dα1;ϑa+z(a)=Iδ;ϑa+z(γ),Dα1;ϑa+z(b)+κz(b)=0. | (4.4) |
Again by Lemma 3.1, we have
˜z(ς)=∫ςaGα1+α2ϑ(ς,s)F(s,˜z(s))ds+λ∫ςaGα1ϑ(ς,s)˜z(s)ds+μ(ς)∫ξaGδϑ(ξ,s)F(s,˜z(s))ds+ν(ς){λ(κ−λ)∫baGα1ϑ(b,s)˜z(s)ds−(κ−λ)∫baGα1+α2ϑ(b,s)F(s,˜z(s))ds−∫baGα2ϑ(b,s)F(s,˜z(s))ds−ϖ∫ξaGδϑ(ξ,s)˜z(s)ds}+∫ςaGα1+α2ϑ(ς,s)ϱ(s)ds+μ(ς)∫ξaGδϑ(ξ,s)ϱ(s)ds+ν(ς){(λ−κ)∫baGα1+α2ϑ(b,s)ϱ(s)ds−∫baGα2ϑ(b,s)ϱ(s)ds}. | (4.5) |
On the other hand, for any ς∈J
|˜z(ς)−z(ς)|≤∫ςaGα1+α2ϑ(ς,s)|ϱ(s)|ds+ν∗|κ−λ|∫baGα1+α2ϑ(b,s)|ϱ(s)|ds+ν∗∫baGα2ϑ(b,s)|ϱ(s)|ds+∫ςaGα1+α2ϑ(ς,s)|F(s,ϰ(s))−F(s,z(s))|ds+|λ|∫ςaGα1ϑ(ς,s)|ϰ(s)−z(s)|ds+μ∗∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds+ν(ς){|λ(κ−λ)|∫baGα1ϑ(b,s)|ϰ(s)−z(s)|ds+(κ−λ)∫baGα1+α2ϑ(b,s)|F(s,ϰ(s))−F(s,z(s))|ds+∫baGα2ϑ(b,s)|F(s,ϰ(s))−F(s,z(s))|ds+ϖ∫ξaGδϑ(ξ,s)|ϰ(s)−z(s)|ds}. |
Using part (i) of Remark 4.3 and (H2), we get
|˜z(ς)−z(ς)|≤((ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)[ν∗|κ−λ|+1]+ν∗(ϑ(b)−ϑ(a))α2Γ(α2+1))ε+Δ‖˜z−z‖, |
where Δ is defined by (3.11). In consequence, it follows that
‖˜z−z‖∞≤((ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)[ν∗|κ−λ|+1](1−Δ)+ν∗(1−Δ)(ϑ(b)−ϑ(a))α2Γ(α2+1))ε. |
If we let cF=((ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)[ν∗(κ−λ)+1](1−Δ)+ν∗(1−Δ)(ϑ(b)−ϑ(a))α2Γ(α2+1)), then, the U-H stability condition is satisfied. More generally, for CF(ε)=((ϑ(b)−ϑ(a))α1+α2Γ(α1+α2+1)[ν∗|κ−λ|+1](1−Δ)+ν∗(1−Δ)(ϑ(b)−ϑ(a))α2Γ(α2+1))ε; CF(0)=0 the generalized U-H stability condition is also fulfilled.
This section is intended to illustrate the reported results with relevant examples.
Example 5.1. We formulate the system of FLDE in the frame of Caputo type:
{ cD1.20+( cD2.50++0.4)z(ς)=1eς+9(1+|z(ς)|1+|z(ς)|),ς∈[0,1],z(0)=0,z′(0)=0,z′′(0)=0,D1.2;ς0+z(0)=I0.5;ϑ0+z(0.1),D1.2;ς0+z(1)+0.5z(1)=0. | (5.1) |
In this case we take
α1=2.5,α2=1.2,λ=0.4,κ=0.5,δ=0.5,ξ=0.1,a=0,b=1,ϑ(ς)=ςandF(ς,z)=1eς+9(1+|z(ς)|1+|z(ς)|). |
Obviously, the hypothesis (H1) of the Theorem 3.4 is fulfilled. On the opposite hand, for each ς∈[0,1],z,ϰ∈R we have
|F(ς,z)−F(ς,ϰ)|≤110|z−ϰ|. |
Hence, (H2) holds with L=0.1. Thus, we find that Δ=0.7635<1. Since all the assumptions in Theorem 3.4 hold, the FLDE (5.1) has a unique solution on [0,1]. Moreover, Theorem 4.4 ensures that the FLDE (1.3) is U-H stable and generalized U-H stable.
Example 5.2. We formulate the system of FLDE in the frame of Hadamard type:
{ HD1.5;lnς1+( HD2.7;lnς1++0.18)z(ς)=1(ς+1)2(1+sinz(ς)),ς∈[1,e],z(1)=0,z′(1)=0,z′′(1)=0, HD1.5;lnς1+z(1)= HI0.9;lnς1+z(2), HD1.5;lnς1+z(e)+0.2z(e)=0. | (5.2) |
Here
F(ς,z(ς))=15(ς+1)2(1+sinz(ς)). | (5.3) |
Obviously, the assumption (H1) of the Theorem 3.4 holds. On the other hand, for any ς∈[1,e],z,ϰ∈R we get
|F(ς,z)−F(ς,ϰ)|≤110|z−ϰ|. |
Consequently, (H2) holds with L=0.1. Besides, by computation directly we find that Δ=0.8731<1.
To illustrate Theorem 3.5, it is clear that the function f satisfies (H1) and (H3) with ‖h‖=0.1. In addition, Λ3≈0.7823<1. It follows from theorem 3.5 that the FLDE (5.2) has a unique solution on [1,e].
Example 5.3. We formulate the system of FLDE in the frame of ϑ-Caputo type:
{ cD1.9;ϑ0+( cD2.9;ϑ0++0.25)z(ς)=eς4(eς+1)(1+arctanz(ς)),ς∈[0,1],z(0)=0,z′(0)=0,z′′(0)=0,Dα1;ϑ0+z(0)=I5.4;ϑa+z(0.3),Dα1;ϑ0+z(1)+0.1z(1)=0. | (5.4) |
Take
α1=1.9,α2=2.5,λ=0.25,δ=5.4,κ=0.1,ξ=0.3,a0=0,b0=1,ϑ(ς)=eς |
F(ς,z)=eς4(eς+1)(1+arctanz(ς)). | (5.5) |
For any ς∈[0,1],z,ϰ∈R we obtain
|F(ς,z)−F(ς,ϰ)|≤18|z−ϰ|. |
Hence, (H2) holds with L=0.125. Moreover, by computation directly we find that Δ=0.7133<1. It follows from Theorem 3.4 that FLDE (5.4) has a unique solution on [0,1].
To illustrate Theorem 3.5, it is clear that the function F(ς,z) given by (5.5) satisfies the hypotheses (H1)–(H3) with ‖h‖=0.125. and Λ3≈0.3247<1. It follows from Theorem 3.5 that the FLDE (5.2) has a unique solution on [0,1].
In this reported article, we have considered a class of nonlinear Langevin equations involving two different fractional orders in the frame of Caputo function-dependent-kernel fractional derivatives with antiperiodic boundary conditions. The existence and uniqueness results are established for the suggested problem. Our perspective is based on properties of ϑ-Caputo's derivatives and applying of Krasnoselskii's and Banach's fixed point theorems. Moreover, we discuss the Ulam-Hyers stability criteria for the at-hand problem. Some related examples illustrating the effectiveness of the theoretical results are presented. The results obtained are recent and provide extensions to some known results in the literature. Furthermore, they cover many fractional Langevin equations that contain classical fractional operators.
This research was funded by the Deanship of Scientific Research at Princess Nourah bint Abdulrahman University, Saudi Arabia through the Fast-track Research Funding Program.
The authors declare that there is no conflict of interests regarding the publication of this paper.
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