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Investigating a generalized Hilfer-type fractional differential equation with two-point and integral boundary conditions

  • In this paper, we investigate a nonlinear generalized fractional differential equation with two-point and integral boundary conditions in the frame of κ-Hilfer fractional derivative. The existence and uniqueness results are obtained using Krasnoselskii and Banach's fixed point theorems. We analyze different types of stability results of the proposed problem by using some mathematical methodologies. At the end of the paper, we present a numerical example to demonstrate and validate our findings.

    Citation: Saleh S. Redhwan, Sadikali L. Shaikh, Mohammed S. Abdo, Wasfi Shatanawi, Kamaleldin Abodayeh, Mohammed A. Almalahi, Tariq Aljaaidi. Investigating a generalized Hilfer-type fractional differential equation with two-point and integral boundary conditions[J]. AIMS Mathematics, 2022, 7(2): 1856-1872. doi: 10.3934/math.2022107

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  • In this paper, we investigate a nonlinear generalized fractional differential equation with two-point and integral boundary conditions in the frame of κ-Hilfer fractional derivative. The existence and uniqueness results are obtained using Krasnoselskii and Banach's fixed point theorems. We analyze different types of stability results of the proposed problem by using some mathematical methodologies. At the end of the paper, we present a numerical example to demonstrate and validate our findings.



    Fractional differential equations (FDEs) provide more advantages than integer-order differential equations. When it comes to explaining the changing laws of nature, these equations are both flexible and exact. As a result, FDEs are commonly used in real-world situations [1-3]. However, the development of the theory of FDEs is still in its early stages because various physical interpretations of FDEs are still unknown due to the intricacies of their initial values. Nonetheless, these equations have become a valid topic of debate among a number of researchers due to their wide range of practical applications and theoretical significance. Atangana and Baleanu [4] introduced a new definition of fractional derivatives with the nonlocal and non-singular kernel. In contrast, the properties of this operator, such as convolution of the power law, exponential decay law, and generalized Mittag-Leffler law with fractal derivative, are introduced by Atangana in [5]. For more details about the application of the Atangana-Baleanu operator see [6]. Zhu [7] studied the stabilization problem of stochastic nonlinear delay systems. Also, Zhu et al. [8] discussed the moment exponential stability problem for a class of stochastic delay nonlinear systems. Hu et al. [9] studied the Razumikhin stability theorem for a class of impulsive stochastic delay differential systems. In the last three decades, some researchers introduced definitions of fractional calculus, including definitions of Riemann-Liouville (RL) and Caputo, and less well-known definitions such as Erdelyi-Kober and Hadamard. In [10], Hilfer was given generalization of FDs of RL and Caputo, which so-called the Hilfer FD of order η and a type q[0,1]. When we give q=0 and q=1 respectively in the formula of Hilfer FD can get RL and Caputo FDs. Such a derivative interpolate between the RL and Caputo FDs. For more details on this FD above-mentioned can be found in [11,12]. In 2018, Sousa and de Oliveira [13] introduced a new FD with respect to another function ψ called "ψ-Hilfer FD" generalizes most of the previous FDs. Some of the existence and stability results of fractional boundary value problems (BVPs) are addressed in the recent literature; for instance, Benchohra et al. [14] studied the existence of solutions of a class of BVPs for a nonlinear FDE

    {CDαυ(σ)=f(σ,υ(σ)),σ[0,T],aυ(0)+bυ(T)=c, (1.1)

    where 0<α<1, a,b,cR, a+b0, and CDα is the Caputo FD of order α. Salim et al. [15] discussed some existence and Ulam stability results for the implicit problem (1.1) with Caputo-Fabrizio FD. Ashyralyev et al. [16] studied the existence and uniqueness of a fractional BVP of the form

    {CDαυ(σ)=f(σ,υ(σ)),σ[0,b],Aυ(0)+Bυ(b)=b0g(s,υ(s))ds, (1.2)

    where 0<α1, CDα is the Caputo FD of order α, A,BRn×n, f,g:[0,b]×RnRn are continuous. Sharifov et al. [17] investigated the existence and uniqueness of the solutions to the following fractional BVP

    {CDαυ(σ)=f(σ,υ(σ)),σ[0,b],Aυ(0)+b0n(s)υ(s)ds+Bυ(b)=C, (1.3)

    where 0<α<1, CDα is the Caputo FD of order α, A,B,CRn×n, f:[0,b]×RnRn is continuous, and n(s):[0,b]Rn×n is given matrices.

    On the other hand, Sousa and de Oliveira [18] proved the existence and uniqueness of solutions of the following Cauchy-type problem

    {Dα,β,ψa+υ(σ)=f(σ,υ(σ)),σ(a,b],I1γ,ψυ(σ)=υa, γ=α+β(1α), (1.4)

    where 0<α<1, 0β1, υaR, Dα,β,ψa+ is the ψ-Hilfer FD, and f:[0,b]×RR is continuous. The authors in [19] discussed the Ulam-Hyers (UH) stability of (1.4) for an integro-differential-type. Furthermore, they proved the Ulam-Hyers-Rassias stability results of (1.4) for an implicit type in [20]. Abdo et al., in [21,22] investigated the existence and various types of stability theorems of fractional Cauchy problem involving ψ-Hilfer FD, whereas, some qualitative analyses of ψ-Hilfer type nonlocal Cauchy problem have been investigated in [23]. Nonlocal fractional BVPs with ψ-Hilfer FDs have been considered in [24,25].

    In this paper, we study the existence, uniqueness and UH stability results of the class of BVPs for the following nonlinear FDE

    {HDη,q;κυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d4, (1.5)

    where 0<η<1, 0q1, HDη,q;κ is the κ-Hilfer FD of order η, and type q, ϝ:J×RR is continuous, diR (i=1,2,3,4), κ(σ)C1(J,R) be an increasing function with κ(σ)0 for all σJ.

    We concentrate on non-local problems because, in many cases, the non-local condition better captures physical phenomena than classical initial (border) conditions. So, utilising Banach's and Krasnoseliskii's fixed point theorems under the minimum assumptions, we analyze the result of existence and uniqueness as well as UH stability results of the BVP (1.5). The work presented in this article is current and adds to the literature, particularly in the area of nonlinear problems of the κ-Hilfer type.

    In general, our results remain valid for various values of the function κ and cover many corresponding problems, for instance (Hilfer-Hadamard type problem for κ(σ)=logσ), (Hilfer-Katugampola type problem for κ(σ)=σρ, ρ>0), (Caputo-type problem for κ(σ)=σ, and q=1), and (RL-type problem for κ(σ)=σ, and q=0).

    The content of this paper is organized as follows: Section 2 presents some required results and preliminaries about κ-Hilfer FD. Our main results for the κ-Hilfer type BVP (1.5) are addressed in Section 3. Some examples to explain the acquired results are constructed in Section 4. Ultimately, we summarize our work in the conclusion section and suggest future directions.

    We set notations and certain fundamental facts in this part, which will be used in the proofs of the following results.

    Let C(J,R) and L(J,R) are the Banach space of continuous functions and Lebesgue integrable functions from J into R with the norms

    υ=sup{|υ|:σJ}, and
    υL=ba|υ(σ)|dσ,

    respectively.

    Definition 2.1. [1] Let η>0 and gL1(J,R). The following expression

    Iη;κg(σ)=1Γ(η)σaκ(t)(κ(σ)κ(t))η1g(t)dt,

    is called left sided κ-RL fractional integral of order η.

    Definition 2.2. [13] The κ-Hilfer FD of order η and parameter q is defined by

    HDη,q;κg(σ)=Iq(nη);κ(1κ(σ)ddσ)n I(1q)(nη);κg(σ),

    where n1<η<n, 0q1, σ>a.

    Lemma 2.3. [1,13] Let η,χ, and δ>0. Then

    (1) Iη;κIη;χg(σ)=Iη+χ;κg(σ).

    (2) Iη;κ(κ(σ)κ(a))δ1=Γ(δ)Γ(η+δ)(κ(σ)κ(a))η+δ1.

    We note also that HDη,q;κ(κ(σ)κ(a))γ1=0.

    Lemma 2.4. [13] Let gL(a,b), η(n1,n] (nN), q[0,1], then

    (Iη;κHDη,q;κg)(σ)=g(σ)nk=0(κ(σ)κ(a))γkΓ(γk+1)g[nk]κI(1q)(nη);κg(a),

    where g[nk]κ=(1κ(σ)ddσ)[nk]g(σ).

    Lemma 2.5. Let υC(J,R). Then, the unique solution of the κ-Hilfer type BVP (1.5) is given by

    υ(σ)=1ΛΓ(γ)(κ(σ)κ(a))γ1[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iη;κϝ(σ,υ(σ)), (2.1)

    where

    Λ=[d2+γd3(κ(b)κ(a))](κ(b)κ(a))γΓ(γ+1)0, (2.2)

    Proof. Let υ be a solution of the first equation of κ-Hilfer type BVP (1.5). Applying Iη;κ on the first equation of κ-Hilfer type BVP (1.5) with Lemma 2.4, and setting I1η;κυ(a)=c0, we obtain

    υ(σ)=c0Γ(γ)(κ(σ)κ(a))γ1+Iη;κϝ(σ,υ(σ)), (2.3)

    where c0, is an arbitrary constant. From condition d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d4, we have

    d4=d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d2baκ(s)[c0Γ(γ)(κ(s)κ(a))γ1+Iη;κϝ(s,υ(s))]ds+d3[c0Γ(γ)(κ(b)κ(a))γ1+Iη;κϝ(b,υ(b))]=c0Γ(γ)[d2baκ(s)(κ(s)κ(a))γ1ds+d3(κ(b)κ(a))γ1]+d2baκ(s)Iη;κϝ(s,υ(s))ds+d3Iη;κϝ(b,υ(b))=c0[d2+γd3(κ(b)κ(a))](κ(b)κ(a))γΓ(γ+1)+d2baκ(s)Iη;κϝ(s,υ(s))ds+d3Iη;κϝ(b,υ(b)).

    Hence

    c0,=1Λ[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))].

    Therefore,

    υ(σ)=1ΛΓ(γ)(κ(σ)κ(a))γ1[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iη;κϝ(σ,υ(σ)).

    This completes the proof.

    Here we can suffice to refer to Banach's fixed point theorem [26] and Krasnoselskii's fixed point theorem [27].

    In this part, we demonstrate the results of the existence and uniqueness of the κ-Hilfer type BVP (1.5) by employing Banach's and Krasnoselskii's fixed point theorems.

    To obtain our main results, the following conditions must be satisfied:

    (H1) The function ϝ is continuous and there exists λ>0 such that

    |ϝ(σ,υ1)ϝ(σ,υ2)|λ|υ1υ2|,

    for any υ1,υ2R and σJ.

    For convenience purpose, we are setting two constant:

    Υ1=λ[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]. (3.1)

    Theorem 3.1. Assume that (H1) holds. Then the κ-Hilfer type BVP (1.5) has at least one solution on J, provided that

    Υ1<1, (3.2)

    where Υ1 was defined by (3.1).

    Proof. In view of Lemma 2.5, we define operator Π:C(J,R)C(J,R) by

    (Πυ)(σ)=(κ(σ)κ(a))γ1ΛΓ(γ)[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(σ,υ(σ))(b)]+Iη;κϝ(σ,υ(σ)).

    Consider the closed ball Bδ={υC(J,R):υδ}, with

    δΥ21Υ1,

    where

    Υ2=N[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]+d4(κ(b)κ(a))γ1ΛΓ(γ),

    and N=maxσJ|ϝ(σ,0)|. Now, we define the operators Π1,Π2 such that Π=Π1+Π2 on Bδ as follows

    (Π1υ)(σ)=Iη;κϝ(σ,υ(σ)), σJ

    and

    (Π2υ)(σ)=(κ(σ)κ(a))γ1ΛΓ(γ)[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(σ,υ(σ))(b)].

    By using (H1), we obtain

    |ϝ(σ,υ(σ))||ϝ(σ,υ(σ))ϝ(σ,0)+ϝ(σ,0)|λ|υ(σ)|+|ϝ(σ,0)|λ|υ(σ)|+N.

    For any υ,υBδ, we have

    (Π1υ)+(Π2υ)supσJ{(κ(σ)κ(a))γ1ΛΓ(γ)[d4+d2baκ(s)Iη;κ|ϝ(s,υ(s))|ds+d3Iη;κ|ϝ(σ,υ(σ))(b)|]+Iη;κ|ϝ(σ,υ(σ))|}(λυ+N)[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)]+d4(κ(b)κ(a))γ1ΛΓ(γ)+(κ(b)κ(a))ηΓ(η+1)(λυ+N)λυ[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]+N[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]+d4(κ(b)κ(a))γ1ΛΓ(γ)λδ[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]+N[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]+d4(κ(b)κ(a))γ1ΛΓ(γ)δΥ1+Υ2δ.

    This shows that Π1υ+Π2υBδ.

    Next, due to continuity of ϝ, we conclude that Π1 is continuous too. Also, Π1 is uniformly bounded on Bδ as

    Π2υ(κ(b)κ(a))ηΓ(η+1)λδ.

    In addition, we prove the compactness of Π1 as follows. Let σ1,σ2J such that σ1<σ2. Then

    |(Π1υ)(σ2)(Π1υ)(σ1)|1Γ(η)|σ1aκ(s)[(κ(σ2)κ(s))η1((κ(σ1)κ(s))η1]|ϝ(s,υ(s))|)ds+σ2σ1κ(s)((κ(σ2)κ(s))η1|ϝ(s,υ(s))|ds|(λδ+N)Γ(η+1)[|(κ(σ2)κ(a))η(κ(σ1)κ(a))η|].

    The last inequality with σ2σ1 0, gives

    |(Π1υ)(σ2)(Π1υ)(σ1)|0, as σ2σ1, υBδ.

    Then, Π1 is relatively compact on Bδ. An application of the Arzel-Ascoli theorem, Π1 is compact on Bδ.

    Now, we will show that Π2 is a contraction. Let υ,υBδ. Then, by (H1) for σJ, we have

    |(Π2υ)(σ)(Π2υ)(σ)|supσJ{(κ(σ)κ(a))γ1ΛΓ(γ)[d4+d2baκ(s)Iη;κ|ϝ(s,υ(s))ϝ(s,υ(s))|ds+d3Iη;κ|ϝ(σ,υ(σ))(b)ϝ(σ,υ(σ))(b)|]}λυυ[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)]Υ1υυ.

    Hence, Π2 is a contraction in Bδ. Thus, all conditions in Krasnoselskii's fixed point theorem are satisfied. So, the κ-Hilfer type BVP (1.5) has at least one solution on J.

    Theorem 3.2. Assume that (H1) holds. Then the κ-Hilfer type BVP (1.5) has unique solution on J, provided that

    Υ1<1, (3.3)

    where Υ1 was defined by (3.1).

    Proof. We shall show that Π has a unique fixed point by using Banach theorem [26]. By Theorem 3.1, we have

    ΠυΠ1υ+Π2υδ.

    Thus, Π(Bδ)Bδ. Now, we show that Π is a contraction. For υ,υBδ and σJ, we have

    (Πυ)(Πυ)(Π1υ)(Π1υ)+(Π2υ)(Π2υ)supσJ{(κ(σ)κ(a))γ1ΛΓ(γ)[d4+d2baκ(s)Iη;κ|ϝ(s,υ(s))ϝ(s,υ(s))|ds+d3Iη;κ|ϝ(σ,υ(σ))ϝ(σ,υ(σ))|]+Iη;κ|ϝ(σ,υ(σ))ϝ(σ,υ(σ))|}λυυ[d2(κ(b)κ(a))η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(κ(b)κ(a))ηΓ(η+1)+(κ(b)κ(a))ηΓ(η+1)]Υ1υυ,

    which implies that ΠυΠυΥ1υυ. By (3.2), we realize that Π is a contraction. Then, by Krasnoselskii Theorem [26], the κ-Hilfer type BVP (1.5) has a unique solution on J.

    Special cases

    According to our previous results, in this subsection we present several special cases:

    Case (1): If κ(σ)=σ, then the κ-Hilfer type BVP (1.5) is reduced to the following Hilfer type problem

    {HDη,qυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baυ(s)ds+d3υ(b)=d4, (3.4)

    where HDη,q,σ is the Hilfer FD of order η, ϝ:J×RR is continuous function, diR (i=1,2,3,4). The solution of the Hilfer type BVP (3.4) is given by

    υ(σ)=(σa)γ1ΛΓ(γ)[d4d2baIηϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iηϝ(σ,υ(σ)),

    where

    Λ=[d2+γd3(ba)](ba)γΓ(γ+1)0.

    Then the following corollary is extracted from the Theorem 3.2.

    Corollary 3.3. Assume that (H1) is satisfied. Then the BVP (3.4) has a unique solution on J provided that Υ1<1, where

    Υ1=λ[d2(ba)η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(ba)ηΓ(η+1)+(ba)ηΓ(η+1)].

    Case (2): If κ(σ)=logσ, then the κ-Hilfer type BVP (1.5) is reduced to the following Hilfer-Hadamard type problem

    {HDη,q,logσυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baυ(s)ds+d3υ(b)=d4, (3.5)

    where HDη,q,logσ is the Hilfer-Hadamard FD of order η, ϝ:J×RR is continuous function, diR (i=1,2,3,4). The solution of the Hilfer-Hadamard type BVP (3.5) is given by

    υ(σ)=(logσa)γ1ΛΓ(γ)[d4d2baIη;logσϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iη;logσϝ(σ,υ(σ)),

    where

    Λ=[d2+γd3(logba)](logba)γΓ(γ+1)0.

    Then the following corollary is deduced from the Theorem 3.2.

    Corollary 3.4. Assume that (H1) is satisfied. Then the BVP (3.5) has a unique solution on J provided that Υ1<1, where

    Υ1=λ[d2(logba)η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(logba)ηΓ(η+1)+(logba)ηΓ(η+1)].

    Case (3): If κ(σ)=σρ,ρ>0, then the κ- Hilfer type BVP (1.5) is reduced to the following Hilfer-Katugumpola type problem

    {HDη,q,σρυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baυ(s)ds+d3υ(b)=d4, (3.6)

    where HDη,q,σρ is the Hilfer-Katugumpola FD of order η,ρ>0, ϝ:J×RR is continuous function, diR (i=1,2,3,4). The solution of the Hilfer-Katugumpola type BVP (3.6) is given by

    υ(σ)=(σρaρ)γ1ΛΓ(γ)[d4d2baIη,σρϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iη,σρϝ(σ,υ(σ)),

    where

    Λ=[d2+γd3(bρaρ)](bρaρ)γΓ(γ+1)0.

    Then the next corollary is a special case of the Theorem 3.2.

    Corollary 3.5. Assume that (H1) is satisfied. Then the BVP (3.6) has a unique solution on J provided that Υ1<1, where

    Υ1=λ[d2(bρaρ)η+γΛΓ(γ)Γ(η+2)+d3ΛΓ(γ)(bρaρ)ηΓ(η+1)+(bρaρ)ηΓ(η+1)].

    In this part, we discuss various types of stability like UH, GUH, UHR and GUHR. First of all, we introduce the following definitions. Let ϵ>0 such that

    |HDη,q;κ¯υ(σ)ϝ(σ,¯υ(σ))|ϵ, (4.1)
    |HDη,q;κ¯υ(σ)ϝ(σ,¯υ(σ))|ϵδκ(σ),δκC(J,R). (4.2)

    Definition 4.1. Let ¯υC(J,R) be a function satisfies (4.1) corresponding to a solution υC(J,R) of κ-Hilfer type BVP (1.5). If there exists 0<TR such that

    |¯υ(σ)υ(σ)|Tϵ,σJ, ϵ>0,

    then,

    HDη,q;κ¯υ(σ)=ϝ(σ,¯υ(σ)), (4.3)

    is UH stable.

    Remark 4.2. A function ¯υC(J,R) satisfies (4.1) if and only if there exist a functions zC(J,R) such that

    (i) |z(σ)|ϵ, σJ,

    (ii) HDη,q;κ¯υ(σ)=ϝ(σ,¯υ(σ))+z(σ), ϰJ.

    Lemma 4.3. If υC(J,R) is a solution to inequality (4.1), then υ satisfies the following inequality

    |υ(σ)Θυ|ϵΠ,

    where

    Θ¯υ=1ΛΓ(γ)(κ(σ)κ(a))γ1[d4d2baκ(s)Iη;κϝ(s,υ(s))dsd3Iη;κϝ(b,υ(b))]+Iη;κϝ(σ,υ(σ)),

    and

    Π=(1ΛΓ(γ)[d4ϵ+d2(κ(b)κ(a))η+γΓ(η+2)+d3(κ(b)κ(a))ηΓ(η+1)]+(κ(b)κ(a))ηΓ(η+1))

    Proof. In view of Remark 4.2, we have

    HDη,q;κυ(σ)=ϝ(σ,υ(σ))+z(ϰ)d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d4.

    Then, by Lemma 2.5, we get

    υ(σ)=Θυ+(κ(σ)κ(a))γ1ΛΓ(γ)[d4d2baκ(s)Iη;κz(s)dsd3Iη;κz(b)]+Iη;κz(σ),

    which implies

    |υ(σ)Θυ|ϵΛΓ(γ)(κ(b)κ(a))γ1[d4ϵ+d2(κ(b)κ(a))ηΓ(η+1)+d3(κ(b)κ(a))ηΓ(η+1)]+ϵ(κ(b)κ(a))ηΓ(η+1)ϵ(1ΛΓ(γ)[d4ϵ+d2(κ(b)κ(a))η+γΓ(η+2)+d3(κ(b)κ(a))ηΓ(η+1)]+(κ(b)κ(a))ηΓ(η+1))ϵΠ.

    Theorem 4.4. Assume that (H1) holds. Under the Lemma 4.3, the following equation

    HDη,q;κυ(σ)=ϝ(σ,υ(σ)),σ[a,b], (4.4)

    is UH stable as well as GUH provided that Υ1<1.

    Proof. ¯υC(J,R) be a function satisfies (4.1), let υC(J,R) be the unique solution of the following problem

    {HDη,q;κυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d4,υ(σ)=¯υ(σ),σJ:=[a,b].

    Then, by Lemma 2.5, we get

    υ(σ)=Θυ.

    It follows from Theorem 3.2, that

    υ¯υ=supσJ|υ(σ)Θ¯υ|supτf|υ(σ)Θυ|+supτf|ΘυΘ¯υ|ϵΠ+Υ1υ¯υ.

    Thus

    υ¯υTϵ,

    where

    T=Π1Υ1>0.

    Now, by choosing φΥ(ϵ)=CΥϵ such that φΥ(0)=0, then the problem (4.4) is GUH stability.

    To prove the Ulam-Heyrs-Rassias stability, we need the following hypotheses:

    (H2) There exists an increasing function δκC(J,R) and there exists W>0 such that for any σJ

    Iη;κδκ(σ)Wδκ(σ). (4.5)

    Definition 4.5. Let ¯υC(J,R) be a function satisfies inequality (4.2) corresponding to a solution υC(J,R) of κ-Hilfer type BVP (1.5). If there exists 0<NR and non-decreasing function δκ(σ) such that

    υ¯υNϵδκ(σ),τf, ϵ>0,

    then, the problem (4.4) is UHR stable with respect to δκ(σ).

    Remark 4.6. A function ¯υC(J,R) satisfies (4.2) if and only if there exist a functions zC(J,R) such that

    (i)|z(τ)|ϵδκ(σ), σJ,

    (ii)HDη,q;κ¯υ(σ)=ϝ(σ,¯υ(σ))+z(τ), τf.

    Lemma 4.7. If υC(J,R) is a solution to inequality (4.2), then υ satisfies the following inequality

    υ(σ)ΘυϵWδκ(σ),

    Proof. Indeed, by Remark 4.6 and Lemma 2.5, one can easily prove that

    υ(σ)ΘυϵWδκ(σ),

    where

    W=(1ΛΓ(γ)[d4ϵ+d2κ(b)+d3]+1).

    Theorem 4.8. Suppose that (H1) and (H2) are satisfied. If Υ1<1, then Eq (4.4) is UHR and generalized UHR stable.

    Proof. Let ¯υ be satisfies (4.2), let ¯υC(J,R) be unique solution of the following problem

    {HDη,q;κυ(σ)=ϝ(σ,υ(σ)),σJ:=[a,b],d1υ(a)+d2baκ(s)υ(s)ds+d3υ(b)=d4,υ(σ)=¯υ(σ),σJ:=[a,b].

    Then, by Lemma 2.5, we get

    υ(σ)=Θυ,

    It follows from Theorem 3.2, that

    υ¯υ=supσJ|υ(σ)Θ¯υ|supσJ|υ(σ)Θυ|+supτf|ΘυΘ¯υ|ϵWδκ(σ)+Υ1υ¯υ.

    Thus

    υ¯υNϵδκ(σ),

    where

    N=W1Υ1>0.

    Hence, the problem (4.4) is UHR stable as well as generalized UHR stable.

    In the end, we support our main results by suggesting an example to show the applicability of the outcomes numerically. In fact, the reported results acquired in Theorems 3.1, 3.2, 4.4 and 4.8 are guaranteed by an example.

    Example 5.1. Consider the following problem

    {HD13,56;σ+1υ(σ)=(σ9)|υ(σ)|1+|υ(σ)|+12,σ[1,32],110υ(1)+2532112σ+1υ(σ)dσ+57υ(32)=1, (5.1)

    where

    η=13,q=56, κ(σ)=σ+1, J=[1,32],
    d1=110,d2=25,d3=57,d4=1.

    From these settings, we compute constants as γ=89, Λ=0.890. For υ1,υ2R+, we have

    |ϝ(σ,υ1)ϝ(σ,υ2)|=(σ9)|υ11+υ1υ21+υ2|(σ9)|υ1υ2|16|υ1υ2|.

    Hence, (H1)holds with λ=16>0. Also, the condition (3.2) is fulfilled, i.e. Υ1=0.18<1. Therefore, by the applying Banach's fixed point theorem, we conclude that the problem (5.1) has a unique solution υ on [1,32]. Finally, we see that the inequality

    |HDη,q;κ¯υ(σ)ϝ(σ,¯υ(σ))|ϵ

    is satisfied. Then the Eq (5.1) is Ulam-Hyers stable with

    υ¯υTϵ,σJ, ϵ>0,

    where

    T=Π1Υ1>0,
    Π=(1ΛΓ(γ)[d4ϵ+d2(κ(b)κ(a))η+γΓ(η+2)+d3(κ(b)κ(a))ηΓ(η+1)]+(κ(b)κ(a))ηΓ(η+1))>0,

    and Υ1=0.18<1. Finally, we consider δκ(σ)=κ(σ)κ(a), for σ[1,32]. Then, δκ:[1,32]R is continuous nondecreasing function. Hence by Lemma 2.3, we get

    Iη;κa+δκ(σ)=Iη;κa+(κ(σ)κ(a))=Γ(2)Γ(η+2)(κ(σ)κ(a))η+1[κ(32)κ(1)]ηΓ(η+2)δκ(σ)=Wδκ(σ), for all ϰJ,

    where W=[κ(32)κ(1)]ηΓ(η+2)>0. Therefore, Theorem 4.8 applicable. Moreover, for ϵ>0 and a continuous function δκ:[1,32]R+ we find that

    |HDη,q;κ¯υ(σ)ϝ(σ,¯υ(σ))|ϵδκ(σ)

    is satisfied. Then Eq (5.1) is UHR stable with

    υ¯υNϵδκ(σ)

    where

    N=W1Υ1>0.

    In this research work, a newly nonlinear fractional differential equation with two-point and integral boundary conditions in the κ-Hilfer fractional derivative frame has been investigated. The existence and uniqueness results of the κ-Hilfer type BVP (1.5) have been obtained using Krasnoselskii and Banach's fixed point theorems. Different types of stability of the κ-Hilfer type BVP (1.5) have been discussed by using some mathematical methodologies. An example is presented to confirm the viability of our obtained results.

    The acquired results in this paper are more general and cover many of the parallel problems that contain special cases of function κ, because our proposed system contains a global fractional derivative that integrates many classic fractional derivatives, for instance, the κ-Hilfer type BVP (1.5) for various values of a function κ and parameter q includes the study of a problem of FDEs involving the Hilfer, Hadamard, Katugampola, and many other fractional derivative operators which are described in the introduction. In future work, we will extend this work by replacing the constants di (i=1,2,3,4) with matrices.

    The authors would like to thank Prince Sultan University for funding this research work.

    The authors declare that they have no conflict of interest.



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