This manuscript is devoted to investigate a class of multi terms delay fractional order impulsive differential equations. Our investigation includes existence theory along with Ulam type stability. By using classical fixed point theorems, we establish sufficient conditions for existence and uniqueness of solution to the proposed problem. We develop some appropriate conditions for different kinds of Ulam-Hyers stability results by using tools of nonlinear functional analysis. We demonstrate our results by an example.
Citation: Amjad Ali, Kamal Shah, Dildar Ahmad, Ghaus Ur Rahman, Nabil Mlaiki, Thabet Abdeljawad. Study of multi term delay fractional order impulsive differential equation using fixed point approach[J]. AIMS Mathematics, 2022, 7(7): 11551-11580. doi: 10.3934/math.2022644
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This manuscript is devoted to investigate a class of multi terms delay fractional order impulsive differential equations. Our investigation includes existence theory along with Ulam type stability. By using classical fixed point theorems, we establish sufficient conditions for existence and uniqueness of solution to the proposed problem. We develop some appropriate conditions for different kinds of Ulam-Hyers stability results by using tools of nonlinear functional analysis. We demonstrate our results by an example.
Fractional calculus has gotten considerable attention recently. Derivatives and integrals of non-integer order are increasingly using for different analysis of various problems. Fractional differential operators are global in nature and preserve greater degree of freedom. Therefore, researchers now give preference to use fractional order differential equations (FODEs) in mathematical modelings of various real world process and phenomenons over classical order differential equation. FODEs have multi-dimensional applications in the variety of fields of modern sciences, such as to control the phase difference in oscillators, to accomplish the high frequency oscillation and in electric engineering DC converter models are used to obtain good assessment of the power conversion efficiency. Recently various biological models have been investigated by using fractional order differential equations. In the mentioned study, researchers have established more good results than those already derived for ordinary differential equations. For some more applications of fractions derivatives, for theory and applications of FODEs see [1,2], for integro-FODEs, see [3]. For basic theory and applications we refer [4]. Some generalized type FODEs have been analyzed in [5,6]. Some engineering applications have been investigated in [7]. For real world applications by using FODEs, see [8]. Those differential equations which observe impulsive conditions at points of discontinuity of solution are known as impulsive differential equations. Impulsive differential equations are the tools used for modeling of those evolutionary and physical phenomena that containing sudden changes and discontinuous jumps. Therefore, the proposed types of impulsive differential equations play a significant role to models such phenomena, in this regards (see [9]). Some stability results about the said area has been studied in [10]. Also some conformable impulsive FODEs have been studied in [11]). In some circumstance physical problems depends on preceding states of problem and cannot be describes by current time. In order to avoid such circumstance, researches introduced an important class of differential equations (DEs) known as Delay Differential Equations (DDEs). There are verities of DDEs including proportional (pantograph), continuous and discrete type DDEs. The concern types of DEs are widely using to formulate various real world phenomena in different fields, such as dynamics, quantum mechanics [12], biology [13], and electrodynamics [14].
Important aspects of mathematical analysis are existence theory and stability analysis. Researchers have used various tools of nonlinear analysis for investigating the existence and uniqueness of solution to various problems of FODEs. Various fixed point results and degrees theories have been developed to investigate the said area for existence of solutions. In same line stability analysis of FODEs has also been given proper attention recently. The mentioned analysis is important for developing various numerical methods. Stability results have been investigated by using various methods including exponential method, Mittag-Leffler method and Hyers-Ulam method (see some detail in [15]). Here, we remark that the Ulam's type stability analysis has given more attention recently. The aforementioned stability results have been derived for various problems of FODEs in last few years (for instance see [16]). Hyers and Ulam had been introduced the mentioned stability for the first time for functional equations in 1940 (see some detail [17]). Rassias [18] extended the mentioned stability analysis for linear equations. Also Jung [19] extended the Rassias stability results for functional equations in nonlinear analysis.
Motivated from the mentioned work, researchers have been given much attention to investigate the aforesaid stability analysis for various dynamical problems (we refer few as [20,21]). For boundary value problems of FODEs, the mentioned stability has been studied very well (we refer few results as [22,23]). Furthermore, results related to existence theory of solutions to various problems of fractional order mathematical models of epidemiology have been investigated very well (for instance see [24]). The said results have been investigated for TB models in [27]. The Green functions theory using FODEs has been established in [25,26]. Also the mentioned analysis has been studied for those FODEs involving non-singular derivatives (for instance see [28]).
The existence theory has been developed very well for FODEs in last few years. As an example the reader can look at the second order FODE with non local boundary condition on the independent variable [29]. Researchers have been used fixed point theory together with topological degree theory to develop necessary condition for existence of solution for various problems of fractional order differential equations. Furthermore, they have also derived various results related to Ulam type stability for said problems. Here we recall a suitable example which has been studied in [33] as
cDηU(t)=F(t,U(t)),1<η≤2,t∈[0,1],Z1U(0)+Z2U(1)=P1(U),Z3U′(0)+Z4U′(1)=P2(U), | (1.1) |
where Z1,Z2,Z3 and Z4 are members of the set of real numbers, which satisfy the condition given as: Z1+Z2≠0 and Z3+Z4≠0. The function F,P1 and P1 are continuous. The authors initially utilized the tools of fractional calculus as well as nonlinear analysis to transform the aforementioned FDE to corresponding integral equation and then used fixed theory to achieve their aims.
Similarly, in [30] uniqueness and existence of solution have been studied by utilizing the tools of fixed point theory. Authors have investigated the following system of FODEs with anti periodic coupled with non local subsidiary conditions as
αc1Dη1U(t)+αc2Dη2U(t)=H1(t,U(t),Y(t)),αc3Dη3Y(t)+αc4Dη4Y(t)=H2(t,U(t),Y(t)),U(0)+U(1)=n∑j=1κjY(βj),U′(0)+U′(1)=n∑j=1λjY′(βj),Y(0)+Y(1)=n∑j=1κ∗jU(βj),Y′(0)+Y′(1)=n∑j=1λ∗jU′(βj). |
The author have used standard Caputo derivative in the consider problem, where parameters α1,α2,α3,α4,κj,κ∗j,λj and λ∗j are real numbers for j=1,2,…,m and 0<βj<1.
Inspired from by the above discussion, in this research work, we take the following system by extending the problem (1.1) utilizing the concept of [30,31] as
{p∑i=1σicDαiU(t)=H(t,U(t),U(λt)),α1∈(1,2]αi∈(0,1], fori=2,3,…,p,t∈[0,τ],Δ(U(tk))=IkU(tk),Δ(U′(tk))=I∗kU(tk),k=0,1,…,m,a1U(0)+b1U(τ)=g1(U),a2U′(0)+b2U′(τ)=g2(U),al,bl∈Rforl=1,2. | (1.2) |
In the consider problem (1.2), σi∈R for i=1,2,…,p with σ1≠0, and functions g1,g2:PC([0,τ]),R)↦R and non linear function H:[0,τ]×R×R↦R are continuous and τ>0 is real constant. Furthermore, impulsive operators Ik and I∗k are also continuous. In this article, we use tools of fixed point theory and functional analysis to obtain the desired results. Results devoted to the existence and uniqueness of solution are derived by using Banach and Krasnoselskii's fixed point theorems. Also, the results devoted to stability analysis of Ulam type are established by using tools of nonlinear functional analysis. For verification of the obtain results, we give appropriate example.
The rest of the paper is organized as follows: In Section 2, we recall some basic concepts of fractional calculus, while the main results, relying on Krasnoselski's fixed point theorem and Banach contraction principal are presented in Section 3. Section 4 is devoted to stability analysis of the proposed problem (1.2). Section 5 contains illustrative examples for the obtained results. In Section 6, we present conclusion of our findings.
This section of research, is devoted to basic results, theorems and lemmas of FPT and non-linear analysis, which we need for investigation of the main work.
In the present work, we use the following space and norm
PC(J,R)=X={U:J↦R:U∈C(Jk),k=0,1,…,m, and U(t+),U(t−) exist,k=1,2,…,m} |
with norm define as
‖U‖=maxt∈J{|U(t)| U∈PC(J,R):t∈J}, |
where
J0=[0,t1],J1=(t1,t,2],J2=(t2,t3],…,Jm=(tm,τ] and J=[0,τ]. |
Definition 2.1. The integral of fractional order α of a function y(t)∈L[0,d] is denoted by Iαy(t), and defined as
Iαy(t)=∫t0y(χ)Γ(α)(t−χ)1−αdχ. |
Definition 2.2. [32] Fractional order Caputo derivative for a function y(t)∈L1([0,d],R+) on the interval [0,d] is defined as
cDαy(t)=∫t0yn(χ)Γ(n−α)(t−χ)α+1−ndχ, |
where n=⌈α⌉ and ⌈α⌉ is defined to be the smallest integer equal or greater than α.
Lemma 2.1. [34] The relation between fractional order integral and derivative is given as
Iα[cDαy(t)]=A1+A2t+A3t2+A4t3+⋯+Antn−1+y(t), |
where Ai∈R for i=1,2,…,n.
Definition 2.3. The mapping T:X⟶Y on norm linear spaces is continuous and complete, if for each bounded M∈X, ¯T(M)∈Y is compact.
Definition 2.4. [35] Let F(X) be the collection of function (real valued) on (X,d) metric space, be equi-continuous x∈X, if for each ϵ>0, we can find δ>0, such that for every function f∈F(X) and x0∈X, we have |f(x0)−f(x)|<ϵ, whenever d(x0−x)<δ.
Definition 2.5. [35] An operator T on (X,d) metric space into itself is Lipschitz, if ∃c≥0, and d(T(x1),T(x2))≤cd(x2,x1), for each x2,x1∈X, where c is called Lipschitz constant and contraction, if 0<c<1.
Definition 2.6. [35] An operator T from a metric space (X,d) into itself is contraction, if ∃0<c<1, such that d(T(x1),T(x2))≤cd(x1,x2),∀x1,x2∈X.
Theorem 2.7. [35]every mapping(self contraction) T in complete (X,d) metric space has unique fixed point.
Theorem 2.8. [36] Assume that H is a non empty, convex, bounded and closed convex bounded subset of a Banach space X. let J1 and J1 be two operator provide that J1U1+J2U2∈H whenever U,U2∈H, J1 is continuous and compact and J2 is contraction map. Then there is U∈H provide that, U=J1U+J2U.
This section of research work is committed, to integral representation and existence results for the consider class of multi-term fractional delay differential equations. The authors established the expression for integral representation of proposed problem. In order to obtain results for existence and stability analysis the authors used the tools of analysis and fixed point theory.
This subsection of the research work, is devoted the integral representation of the consider model (1.2).
Theorem 3.1. Assumed that Y(t)∈C(J,R), then the solution of multi-term impulsive fractional delay differential equation,
{p∑i=1σicDαiU(t)=Y(t),α1∈(1,2]αi∈(0,1], fori=2,3,…,p,t∈[0,τ],Δ(U(tk))=IkU(tk),Δ(U′(tk))=I∗kU(tk),k=0,1,…,m,a1U(0)+b1U(τ)=g1(U),a2U′(0)+b2U′(τ)=g2(U),al,bl∈Rforl=1,2, | (3.1) |
is equivalent to the integral equation
![]() |
(3.2) |
Where gi(i=1,2):C(J,R)↦R are continuous function, al+bl≠0 for l=1,2 and α1−αi−1>0 for i=2,3,…,p and
D=σ1a1+b1g1(U)+b2σ1a2+b2(t−τb1a1+b1)g2(U)−b1a1+b1[σ1m∑j=1IjU(tj)+σ1m−1∑j=1(tm−tj)I∗jU(tj)+σ1m∑j=1(t−tm)I∗jU(tj)]−b2a2+b2(t−τb1a1+b1)m∑j=11Γ(α1−1)∫tjtj−1(tj−X)α1−2Y(X)dX+b2a2+b2(t−τb1a1+b1)m∑j=1p∑i=2σi1Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2U(X)dX−b2a2+b2(t−τb1a1+b1)1Γ(α1−1)∫τtm(τ−X)α1−2Y(X)dX+b2a2+b2(t−τb1a1+b1)p∑i=2σi1Γ(α1−αi−1)∫τtm(τ−X)α1−αi−2U(X)dX+b1a1+b1[−m∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1Y(X)dX−m∑j=1τ−tmΓ(α1−1)∫tjtj−1(tj−X)α1−2Y(X)dX−m−1∑j=1tm−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2Y(X)dX+m∑j=1p∑i=2σi1Γ(α1−αi)∫tjtj−1(tj−X)α1−αi−1U(X)dX+m∑j=1p∑i=2σiτ−tmΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2U(X)dX−1Γ(α1)∫τtm(τ−X)α1−1Y(X)dX+m−1∑j=1p∑i=2σitm−tjΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2U(X)dX−p∑i=2σi∫τtm(τ−X)α1−αi−1Γ(α1−αi)U(X)dX]. |
Proof. Applying fractional order integral Iα1 on (3.1) and in-view of Lemma 2.1 for t∈[0,t1], we get
σ1U(t)=C0+C1t+1Γ(α1)∫t0(t−X)α1−1Y(X)dX−p∑i=2σiΓ(α1−αi)∫t0(t−X)α1−αi−1U(X)dX. | (3.3) |
By differentiating (3.3), we get
σ1U′(t)=C1+1Γ(α1−1)∫t0(t−X)α1−2Y(X)dX−p∑i=2σiΓ(α1−αi−1)∫t0(t−X)α1−αi−2U(X)dX. | (3.4) |
Similarly, for t∈(t1,t2], the system (3.1) become
σ1U(t)=C01+C11(t−t1)+1Γ(α1)∫tt1(t−X)α1−1Y(X)dX−p∑i=2∫tt1σi(t−X)α1−αi−1Γ(α1−αi)U(X)dX. | (3.5) |
By differentiating (3.5), we get
σ1U′(t)=C11+1Γ(α1)∫tt1(t−X)α1−1Y(X)dX−p∑i=2σiΓ(α1−αi)∫tt1(t−X)α1−αi−1U(X)dX. | (3.6) |
Now to compute σ1U(t−1), σ1U′(t−1), σ1U(t+1) and σ1U′(t+1) using (3.3)–(3.6), we obtain
σ1U(t−1)=C0+C1t1+1Γ(α1)∫t10(t1−X)α1−1Y(X)dX−p∑i=2∫t10σit1−X)α1−αi−1Γ(α1−αi)(U(X)dX,σ1U′(t−1)=C1+1Γ(α1−1)∫t10(t1−X)α1−2Y(X)dX−p∑i=2∫t10σi(t1−X)α1−αi−2Γ(α1−αi−1)U(X)dX,σ1U(t+1)=C01,σ1U′(t+1)=C11. | (3.7) |
Using the impulsive condition
Δ(U(t1))=U(t+1)−U(t−1)=I1U(t1), |
and
Δ(U′(t1))=U′(t+1)−U′(t−1)=I∗1U(t1), |
we get
C01=σ1I1U(t1)+C0+C1t1+1Γ(α1)∫t10(t1−X)α1−1Y(X)dX−p∑i=2σi1Γ(α1−αi)∫t10(t1−X)α1−αi−1U(X)dX,C11=σ1I∗1U(t1)+C1+1Γ(α1−1)∫t10(t1−X)α1−2Y(X)dX−p∑i=2σi1Γ(α1−αi−1)∫t10(t1−X)α1−αi−2U(X)dX. | (3.8) |
Using (3.8) in (3.5), we obtain
![]() |
On the same fashion, for t∈(tk,tk+1], (3.1) becomes
σ1U(t)=C0+tC1+σ1k∑j=1IjU(tj)+σ1k−1∑j=1(tk−tj)I∗jU(tj)+σ1k∑j=1(t−tk)I∗jU(tj)+σ1k∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1Y(X)dX+k∑j=1t−tkΓ(α1−1)∫tjtj−1(tj−X)α1−2Y(X)dX+k−1∑j=1tk−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2Y(X)dX−k∑j=1p∑i=2σi1Γ(α1−αi)∫tjtj−1(tj−X)α1−αi−1U(X)dX−k∑j=1p∑i=2σi(t−tk)Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2U(X)dX+1Γ(α1)∫ttk(t−X)α1−1Y(X)dX−k−1∑j=1p∑i=2σi(tk−tj)Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2U(X)dX−p∑i=2σiΓ(α1−αi)∫ttk(t−X)α1−αi−1U(X)dX. | (3.9) |
By using the boundary conditions involve in (3.1), we obtain
C1=−b2a2+b2[m∑j=1∫tjtj−1(tj−X)α1−2Γ(α1−1)Y(X)dX−m∑j=1p∑i=2∫tjtj−1σi(tj−X)α1−αi−2Γ(α1−αi−1)U(X)dX−p∑i=2∫τtmσi(τ−X)α1−αi−2Γ(α1−αi−1)U(X)dX+1Γ(α1−1)∫τtm(τ−X)α1−2Y(X)dX]+σ1a2+b2g2(U) | (3.10) |
and
![]() |
(3.11) |
One can obtain the desired integral form of solution (3.2), by using (3.10) and (3.11) in (3.9) and (3.3).
Corollary 3.1. In view of Theorem 3.1 the solution of the given multi-terms fractional delay differential equation (1.2) is given by
![]() |
(3.12) |
Where (gi(i=1,2):C(J,R)↦R) are continuous functions, al+bl≠0 for l=1,2 and α1−αi−1>0 for i=2,3,…,p and
![]() |
In this subsection of the research work, we represent the desired solution for MIFDDE (1.2), in the form of operator equation and provides some assumptions for investigation of existence results for proposed problem.
Lets define T:X↦X, such that
![]() |
(3.13) |
We consider the following assumptions, which we needs for further correspondence in this work. (H1) For U1,U2∈X, there exist LF1,LF2≥0, i.e
|H(t,U1(t),U2(λt))−H(t,U2(λt),U2(t))|≤LF1||U1−U2||+LF2||U1−U2||. | (3.14) |
(H2) For U1,U2∈X, there exist Lgi>0, for i = 1, 2, such that
|gi(U1)−gi(U2)|≤Lgi||U1−U2||. | (3.15) |
(H3) For U1,U2∈X, there exist LI>0, such that
|IkU1(t)−IkU2(t)|≤LI||U1−U2||. | (3.16) |
(H4) For U1,U2∈X, there exist LI∗>0, such that
|I∗kU1(t)−I∗kU2(t)|≤LI∗||U1−U2||. | (3.17) |
(H5) For any U∈X, there exist BF:C(J,R+) such that
|H(t,U(t),U(λt))|≤BF(t). | (3.18) |
(H6) For any U∈X, there exist Bgi:C(J,R+) for i=1,2, such that
|gi(U)|≤Bgi(t). | (3.19) |
(H7) For any U∈X, there exist BI:C(J,R+), such that
|IkU(t)|≤BI(t). | (3.20) |
(H8) For any U∈X, there exist BI∗:C(J,R+), such that
|I∗kU(t)|≤BI∗(t). | (3.21) |
For computational convenience, we introduce the following notation:
BI=(|b1||a1+b1|+1)m. | (3.22) |
BI∗=(|b1||a1+b1|+1)τ(2m−1). | (3.23) |
Bg2=|b2||a2+b2|supt∈J{|t−τb1a1+b1|}. | (3.24) |
![]() |
(3.25) |
BC=p∑i=2|σi|τα1−αi|σ1|Γ(α1−αi)(m+1α1−αi+2m−1)+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}p∑i=2(m+1)|σi|Γ(α1−αi)τα1−αi−1+|b1||σ1||a1+b1|p∑i=2|σi|1Γ(α1−αi)τα1−αi(m+1α1−αi+2m−1)). | (3.26) |
L=BILI+BI∗LI∗+Lg1|a1+b1|+Bg2Lg2+BLFLF+BC. | (3.27) |
Ld=BLFLF+BC. | (3.28) |
BLR=BLF−τα1|σ1|Γ(α1+1). | (3.29) |
Theorem 3.2. Consider (H1)–(H4) holds and L<1, then problem (1.2) has at most one fixed point, where L is defined by (3.27).
Proof. Consider that U,U∗∈X and t∈Jk where k = 1, 2…, m.
|T(U(t))−T(U∗(t))|≤1|σ1|[|σ1|k∑j=1LI||U1−U2||+|σ1|k−1∑j=1(tk−tj)LI∗||U1−U2||+|σ1|k∑j=1supt∈J{|t−tk|}LI∗||U1−U2||+|σ1|k∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1(LF1||U1−U2||+LF2||U1−U2||)dX+k∑j=1|t−tk|Γ(α1−1)∫tjtj−1(tj−X)α1−2(LF1||U1−U2||+LF2||U1−U2||)dX+k−1∑j=1tk−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2(LF1||U1−U2||+LF2||U1−U2||)dX+(k∑j=1p∑i=2∫tjtj−1|σi|(tj−X)α1−αi−1Γ(α1−αi)+|σi||t−tk|Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2)||U−U∗||dX+k−1∑j=1p∑i=2|σi|(tk−tj)Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2||U−U∗||dX+supt∈J{p∑i=2∫ttk|σi|(t−X)α1−αi−1Γ(α1−αi)||U−U∗||dX}+supt∈J{1Γ(α1)∫ttk(t−X)α1−1(LF1||U1−U2||+LF2||U1−U2||)dX}]+1|a1+b1||g1(U)−g1(U∗)|+|b2||a2+b2||t−τb1a1+b1||g2(U)−g2(U∗)|+|b1||a1+b1|[m∑j=1LI||U1−U2||+m−1∑j=1(tm−tj)LI∗||U1−U2||+m∑j=1supt∈J{|t−tm|}LI∗||U1−U2||]+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}[m∑j=11Γ(α1−1)∫tjtj−1(tj−X)α1−2(LF1||U1−U2|| |
+LF2||U1−U2||)dX+m∑j=1p∑i=2|σi|1Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2||U−U∗||dX+1Γ(α1−1)∫τtm(τ−X)α1−2(LF1||U1−U2||+LF2||U1−U2||)dX+p∑i=2|σi|1Γ(α1−αi−1)∫τtm(τ−X)α1−αi−2||U−U∗||dX]+|b1||σ1||a1+b1|[m∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1(LF1||U1−U2||+LF2||U1−U2||)dX+m∑j=1τ−tmΓ(α1−1)∫tjtj−1(tj−X)α1−2(LF1||U1−U2||+LF2||U1−U2||)dX+m−1∑j=1tm−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2(LF1||U1−U2||+LF2||U1−U2||)dX+m∑j=1p∑i=2|σi|1Γ(α1−αi)∫tjtj−1(tj−X)α1−αi−1||U−U∗||dX+m∑j=1p∑i=2|σi|τ−tmΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2||U−U∗||dX+1Γ(α1)∫τtm(τ−X)α1−1(LF1||U1−U2||+LF2||U1−U2||)dX+m−1∑j=1p∑i=2|σi|tm−tjΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2||U−U∗||dX+p∑i=2|σi|1Γ(α1−αi)∫τtm(τ−X)α1−αi−1||U−U∗||dX]. | (3.30) |
Let us assume LF=LF1+LF2 and evaluate the integral involve in (3.30), we have
![]() |
(3.31) |
It is quite clearly that tj−1−tj≤τ, hence by using the aforementioned inequality equation (3.31) can be express as
|T(U(t))−T(U∗(t))|≤||U1−U2|||σ1|[LI|σ1|m+LI∗|σ1|τ(2m−1)+LFτα1Γ(α1)(|σ1|m+1α1+2m−1)+p∑i=2|σi|τα1−αiΓ(α1−αi)(m+1α1−αi+2m−1)]+Lg1||U−U∗|||a1+b1|+|b2|Lg2||U−U∗|||a2+b2|supt∈J{|t−τb1a1+b1|}+|b1|||U−U∗|||a1+b1|(mLI+(2m−1)τLI∗)+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}[(m+1)τα1−1Γ(α1)LF+p∑i=2(m+1)|σi|Γ(α1−αi)τα1−αi−1]+|b1|||U−U∗|||σ1||a1+b1|[τα1Γ(α1)(m+1α1+(2m−1))LF+p∑i=2|σi|1Γ(α1−αi)τα1−αi(m+1α1−αi+2m−1))]. | (3.32) |
By rearranging term containing LI, LI∗, Lg1, Lg2 and LF in Eq (3.32), we obtain
![]() |
(3.33) |
Now using (3.22)–(3.27) in (3.33), we have
|T(U(t))−T(U∗(t))|≤||U1−U2||[BILI+BI∗LI∗+Lg1|a1+b1|+Bg2Lg2+BLFLF+BC]≤L‖U−U∗‖. |
Therefore, by Banach contraction principal the mapping T has fixed point. Thus, the consider problem (1.2) has solution, which is unique.
Theorem 3.3. The consider problem (1.2) has at least one solution, if (H1) and (H5)–(H8) holds and Ld<1, where Ld is defined in (3.28).
Proof. In order to prove existence of at least one solution, we define operator T1,T2:PC(J,R)↦PC(J,R) given by
![]() |
and
![]() |
Moreover, we construct a ball H={U(t)∈PC(J,R):‖U‖≤R}, with positive radius R chosen as
R≥1(1−BC)(BI‖BI(t)‖+BI∗||BI∗(t)||+||Bg1(t)|||a1+b1|+Bg2||Bg2(t)||+BLF||BF(t)||). |
Step 1: We claim that T1U1(t)+T2U2(t)∈H⊆PC(J,R) for every U1(t),U2(t)∈H⊆PC(J,R).
Now for the proof of desired results, consider
||T1U1(t)+T2U2(t)||≤k∑j=1||BI(t)||+k−1∑j=1(tk−tj)||BI∗(t)||+k∑j=1supt∈J{|t−tk|}||BI∗(t)||+1|a1+b1|||Bg1(t)||+|b2||a2+b2||t−τb1a1+b1|||Bg2(t)||+|b1||a1+b1|[m∑j=1||BI(t)||+m−1∑j=1(tm−tj)||BI∗(t)||+m∑j=1supt∈J{|t−tm|}||BI∗(t)||]+1|σ1|[|σ1|k∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1||BF(t)||dX+k∑j=1|t−tk|Γ(α1−1)∫tjtj−1(tj−X)α1−2||BF(t)||dX+k−1∑j=1tk−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2||BF(t)||dX+k∑j=1p∑i=2|σi|1Γ(α1−αi)∫tjtj−1(tj−X)α1−αi−1RdX+k∑j=1p∑i=2|σi||t−tk|Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2RdX+k−1∑j=1p∑i=2|σi|tk−tjΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2RdX+supt∈J{1Γ(α1)∫ttk(t−X)α1−1||BF(t)||dX}+supt∈J{p∑i=2|σi|1Γ(α1−αi)∫ttk(t−X)α1−αi−1RdX}]+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}[m∑j=1∫tjtj−1(tj−X)α1−2Γ(α1−1)||BF(t)||dX+∫τtm(τ−X)α1−2Γ(α1−1)||BF(t)||dX+m∑j=1p∑i=2|σi|1Γ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2RdX+p∑i=2|σi|1Γ(α1−αi−1)∫τtm(τ−X)α1−αi−2RdX]+|b1||σ1||a1+b1|[m∑j=11Γ(α1)∫tjtj−1(tj−X)α1−1||BF(t)||dX+m∑j=1τ−tmΓ(α1−1)∫tjtj−1(tj−X)α1−2||BF(t)||dX+m−1∑j=1tm−tjΓ(α1−1)∫tjtj−1(t1−X)α1−2||BF(t)||dX+m∑j=1p∑i=2|σi|1Γ(α1−αi)∫tjtj−1(tj−X)α1−αi−1RdX+m∑j=1p∑i=2|σi|τ−tmΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2RdX+1Γ(α1)∫τtm(τ−X)α1−1||BF(t)||dX+m−1∑j=1p∑i=2|σi|tm−tjΓ(α1−αi−1)∫tjtj−1(tj−X)α1−αi−2RdX+p∑i=2|σi|1Γ(α1−αi)∫τtm(τ−X)α1−αi−1RdX]. | (3.34) |
By using (H5)–(H8), and evaluating the integral in (3.34), we obtain
![]() |
By rearranging term containing LI, LI∗, Lg1, Lg2, and LF in (3.34), we obtain
||T1U1(t)+T2U2(t)||≤(|b1||a1+b1|+1)m||BI(t)||+(|b1||a1+b1|+1)τ(2m−1)||BI∗(t)||+||Bg1(t)|||a1+b1|+|b2||a2+b2|supt∈J{|t−τb1a1+b1|}||Bg2(t)||+{τα1|σ1|Γ(α1)(|σ1|m+1α1+2m−1)+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}(m+1)τα1−1Γ(α1)+|b1||σ1||a1+b1|τα1Γ(α1)(m+1α1+(2m−1))}||BF(t)||+R{p∑i=2τα1−αiΓ(α1−αi)(m+1α1−αi+2m−1)+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}p∑i=2(m+1)|σi|Γ(α1−αi)τα1−αi−1+|b1||σ1||a1+b1|p∑i=2|σi|1Γ(α1−αi)τα1−αi(m+1α1−αi+2m−1))}. | (3.35) |
By using (3.22)–(3.26) in (3.35), we obtain
![]() |
Hence it show that T1U1(t)+T2U2(t)∈H⊆PC(J,R).
Step 2: Here we claim that F1 is uniformly bounded for confirmation, we proceed as
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(3.36) |
As we clearly see that t−tm≤τ. So substitute τ instead of t−tm in (3.36), then we obtain
![]() |
(3.37) |
Using (3.22)–(3.24) in (3.37), we obtain
||T1U1(t)+T2U2(t)||≤BI||BI(t)||+BI∗||BI∗(t)||+||Bg1(t)|||a1+b1|+Bg2||Bg2(t)||. |
Hence T1 is uniformly bounded.
Step 3: Suppose Un(t) is a sequence in H which converge to U∈H for the continuity of T1 we have to prove F1(Un(t))↦T1(U(t)). For the proof we precede as
||T1Un(t)−T1U(t)||≤k∑j=1|IjUn(tj)−IjU(tj)|+k−1∑j=1(tk−tj)|I∗jUn(tj)−I∗jU(tj)|+k∑j=1supt∈J{|t−tk|}|I∗jUn(tj)−I∗jU(tj)|]+1|a1+b1||g1(Un)−g1(U)|+|b2||a2+b2|supt∈J{|t−τb1a1+b1|}|g2(Un)−g2(U)|+|b1||a1+b1|[m∑j=1|IjUn(tj)−IjU(tj)|+m−1∑j=1(tm−tj)|I∗jUn(tj)−I∗jU(tj)|+m∑j=1supt∈J{|t−tm|}|I∗jUn(tj)−I∗jU(tj)|]. |
Hence clearly from the continuity of g1,g2,Ij and I∗j, we get that T1 is continuous.
Step 4: To prove T1 is equi-continuous. Consider
![]() |
clearly as t1↦t2 we have ||T1U(t2)−T1U(t1)||=0. Hence T1 is equi-continuous.
Step 5: To prove T2 is contraction, one can get help from Theorem 3.2 and obtain the following expression,
||T2U1(t)−T2U2(t)||≤||U1−U2||[{τα1(|σ1|m+1α1+2m−1)+|b2||a2+b2|supt∈J{|t−τb1a1+b1|}(m+1)τα1−1|σ1|Γ(α1)+|b1||σ1||a1+b1|τα1Γ(α1)(m+1α1+(2m−1))}LF+{p∑i=2τα1−αiΓ(α1−αi)(m+1α1−αi+2m−1)+|b2||σ1||a2+b2|supt∈J{|t−τb1a1+b1|}p∑i=2(m+1)|σi|Γ(α1−αi)τα1−αi−1+|b1|||U−U∗|||σ1||a1+b1|p∑i=2|σi|1Γ(α1−αi)τα1−αi(m+1α1−αi+2m−1))}]. | (3.38) |
By using (3.25), (3.26) and (3.28) in (3.38), we obtain
||T2U1(t)−T2U2(t)||≤||U1−U2||[BLFLF+BC],≤Ld||U−U∗||. |
Thus all assumption of Krasnoselskii's fixed point theorem are satisfied. So the problem (1.2) has at least one solution.
The authors motivated by the literature [10,29] and present some specific findings for the stability analysis of the proposed problem (1.2).
Definition 4.1. The solution U(t) of proposed problem will be Ulam-Hyres (UH) stable, if for unique solution U∗(t) one can find B1>0, such that for each solution U∈PC(J,R) of the following differential inequality and ϵ>0
{|p∑i=1σicDαiU(t)−f(t,U(t),U(λt))|≤ϵ,t∈[0,τ]|Δ(U(tk))−IkU(tk)|≤ϵ,k=1,2,…,m,|Δ(U′(tk))−I∗kU(tk)|≤ϵ,k=1,2,…,m, | (4.1) |
and a unique solution U∗∈PC(J,R) of the given problem (1.2), such that |U−U∗|≤B1ϵ and solution will be generalized Ulam-Hyers (GUH) stable, if there exist a positive function K:(0,∞)↦(0,∞) with K(0)=0, such that |U−U∗|≤B1K(t).
Definition 4.2. The solution of consider problem is UH Rassias stable, with respect to continuous function χ∈X and a positive constant ψ>0 if we have B2 (positive constant) >0, and ϵ>0, for each solution U∈PC(J,R) of the following differential inequality
{|p∑i=1σicDαiU(t)−f(t,U(t),U(λt))|≤χ(t)ϵ,t∈[0,τ]|Δ(U(tk))−IkU(tk)|≤ψϵ,k=1,2,…,m,|Δ(U′(tk))−I∗kU(tk)|≤ψϵ,k=1,2,…,m, | (4.2) |
and a unique solution U∗∈PC(J,R) of the given problem (1.2), such that |U−U∗|≤B2(χ(t)+ψ)ϵ.
Definition 4.3. The solution of consider problem is GUH Rassias stable, with respect to continuous function χ∈X and a positive constant ψ>0 if we have B2(positive constant) >0, for each solution U∈PC(J,R) of the following differential inequality
{|p∑i=1σicDαiU(t)−f(t,U(t),U(λt))|≤χ(t),t∈[0,τ]|Δ(U(tk))−IkU(tk)|≤ψ,k=1,2,…,m,|Δ(U′(tk))−I∗kU(tk)|≤ψ,k=1,2,…,m. | (4.3) |
and a unique solution U∗∈PC(J,R) of the given problem (1.2), such that |U−U∗|≤B2χ(t)ϵ.
Remark 1. The solution of the inequality (4.1) is U∗∈PC(J,R), iff one can find a function ζ∈PC(J,R), and a sequence ζk,k=1,2,…,m. Depend on U, such that
{(i)ζ(t)≤ϵ,ζk≤ϵwherek=1,2,3,…,m,t∈J(ii)p∑i=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t∈[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,…,m,(iv)Δ(U′(tk))=I∗kU(tk)+ζk,k=1,…,m. | (4.4) |
Remark 2. Let U∗∈PC(J,R) be the solution of (4.2), iff one can find a function ζ∈PC(J,R), and a sequence ζk,k=1,2,…,m. Depend on U, such that
{(i)ζ(t)≤χ(t)ϵ,ζk≤ψϵwherek=1,2,3,…,m,t∈J(ii)p∑i=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t∈[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,…,m,(iv)Δ(U′(tk))=I∗kU(tk)+ζk,k=1,…,m. | (4.5) |
Remark 3. Let U∗∈PC(J,R) be the solution of (4.3), iff one can find a function ξ∈PC(J,R), and a sequence ζk,k=1,2,…,m. Depend on U, such that
{(i)ζ(t)≤χ(t),ζk≤ψwherek=1,2,3,…,m,t∈J(ii)p∑i=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t∈[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,…,m,(iv)Δ(U′(tk))=I∗kU(tk)+ζk,k=1,…,m. | (4.6) |
Lemma 4.1. Consider U∈PC(J,R) is solution of FDDE,
![]() |
(4.7) |
satisfy the following relation,
|U(t)−TU(t)|≤(BI+BI∗+BLF)ϵ. |
Proof. In light of Theorem 3.1, the solution of (4.7), is given as
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(4.8) |
By taking absolute on (4.8) and using Remark 1, we get
![]() |
By using (3.22), (3.23) and (3.25), we obtain
|U(t)−TU(t)|≤(BI+BI∗+BLF)ϵ. |
Which prove the required result.
Theorem 4.4. Under the assumptions (H1–H4), the problem (1.2) is UH as well as GUH stable, if L<1, where L is defined in (3.27).
Proof. For any solution U∈PC(J,R), and unique solution U∗ of the the given problem (1.2), then
||U(t)−U∗(t)||=||U(t)−TU∗(t)||=||U(t)−TU∗+TU−TU||,≤||U(t)−TU||+||TU−TU∗||. |
Using Theorem 3.2 and Lemma 4.1 we have
||U(t)−U∗(t)||≤LUϵ+L||U(t)−U∗(t)||,||U(t)−U∗(t)||−L||U(t)−U∗(t)||≤LUϵ,||U(t)−U∗(t)||≤LU1−Lϵ. |
Let B1=LU1−L, then the solution of the consider problem (1.2) is UH stable further set K(ϵ)=ϵ then the consider problem (1.2) is GUH stable.
To prove the next stability result we need the following assumption given as (H9). For any non decreasing function χ∈PC(J,R+) there exist a positive constant G, such that
1Γ(α1)∫ttk(t−X)α1−1χ(X)dX≤Gχ(t). |
Lemma 4.2. If assumption (H9) holds then for any solution x∈PC(J,R) the muti-term fractional delay differential equation
{p∑i=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),α1∈(1,2]αi∈(0,1], fori=2,3,…,p,t∈[0,τ]Δ(U(tk))=IkU(tk),Δ(U′(tk))=I∗kU(tk),k=0,1,…,m,a1U(0)+b1U(τ)=g1(U),a2U′(0)+b2U′(τ)=g2(U),al,bl∈Rforl=1,2 | (4.9) |
satisfy the following relation,
|U(t)−TU(t)|≤(BI+BI∗+BLR)Aϵ+Gσ1χ(t)ϵ. |
Proof. We omit the proof as it is straightforward and may be derived like Lemma 4.1.
Theorem 4.5. Under the assumption (H1–H4) and H9, the problem (1.2) is UHR stable and GUHR stable, if L<1.
Proof. For any solution U∈PC(J,R), and unique solution U∗ of the the given problem (1.2), then
||U(t)−U∗(t)||=||U(t)−TU∗(t)||=||U(t)−TU∗+TU−TU||≤||U(t)−TU||+||TUd−TU∗||. |
Using Theorem 3.2 and Lemma 4.2, we have
||U(t)−U∗(t)||≤(BI+BI∗+BLR)Aϵ+G|σ1|χ(t)ϵ+L||U(t)−U∗(t)||,||U(t)−U∗(t)||−L||U(t)−U∗(t)||≤(BI+BI∗+BLR)Aϵ+G|σ1|χ(t)ϵ,||U(t)−U∗(t)||≤(BI+BI∗+BLR)A+G|σ1|χ(t)1−Lϵ. |
Let B1=max(BI+BI∗+BLR,G|σ1|)1−L, then the solution of the consider problem (1.2) is UHR stable further set ϵ=1 then the consider problem (1.2) is GUHR stable.
Here we present an example to demonstrate our results.
Example 1. Consider the following multi-term impulsive fractional delay differential equation
{p∑i=11010i−9cD41+2iU(t)=L(3t3+44et+55t)2(2|U(t)|cos(t)+|U(t)|−t3|U(t6)|sec(t)+|U(t8)|−cosh(t)),t∈[0,1],t≠14,L∈R+Δ(U(14))=IkU(14)=|U(14)|32+|U(14)|,Δ(U′(14))=I∗kU(14)=|U(14)|54+|U(14)|,8U(0)+U(1)=g1(U)=|U|100+|U|,6U′(0)+U′(1)=g2(U)=142+|U|, | (5.1) |
here
p=5,m=1,a1=8,b1=b2=1,a2=6,τ=1,τ=1, |
α1=4/3,αi=41+2i,σ1=10,σi=1010i−9. |
|H(t,U(t),U(t6))−f(t,U1(t),U(t6)|≤L(3t3+44et+55t)2(|2|U1(t)|cos(t)+|U1(t)|−2|U2(t)|cos(t)+|U2(t)||+|t3|U1(t6)|sec(t)+|U1(t8)|−t3|U2(t6)|sec(t)+|U2(t8)||)≤L442(2cos(t)|U1(t)−U2(t)|+t3sec(t)|U1(t)−U2(t)|). |
Hence, we obtain LF=L442(2cos(1)+1), and similarly by simple computation, one can calculate,
Lg1=1100,Lg2=11764,LI=132,andLI∗=154. |
Hence, we can calculate that L<1 if G<24.608599. Now as a consequence of Theorem 3.2, we conclude that example 1, has unique solution.
Set χ(t)=(4t−1)2, and ψ=3∀t∈J. since
1Γ(43)∫t14(t−X)43−1(4X−1)2dX=32Γ(133)(t−14)103≤26.3103(4t−1)2 |
condition H9 is satisfied with G=26.3103. Hence all assumption of Theorem 4.5 are satisfied so as a conclusion the solution of problem 1.2 is UHR and GUHR stable. Moreover problem (1.2) is UH and GUH stable due to Theorem 4.4.
In this research work we have established a detailed analysis about existence theory of at least one solution to a class of multi term impulsive FODEs. The required theory has been established by using Krasnoselskii's fixed-point theorem and Banach contraction principle. Also keeping in mind the importance of stability, we have developed some results regarding different kinds of Ulam stability including HU, GHU, HUR and GHUR. The obtained analysis has been demonstrated by using pertinent examples.
Authors Kamal Shah, Nabil Mlaiki and Thabet Abdeljawad would like to thank Prince Sultan University for paying the APC and support through research Lab TAS.
No conflict of interest exists.
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