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Vol. 22 (2021), No. 2, pp. 491–502 DOI: 10.18514/MMN.2021.3470

CONTROLLABILITY AND HYERS-ULAM STABILITY RESULTS OF INITIAL VALUE PROBLEMS FOR FRACTIONAL

DIFFERENTIAL EQUATIONS VIA GENERALIZED PROPORTIONAL-CAPUTO FRACTIONAL DERIVATIVE

MOHAMED I. ABBAS Received 06 October, 2020

Abstract. This paper concerns the investigation of controllability and Hyers-Ulam stability of initial value problems for fractional differential equations via generalized proportional-Caputo fractional derivatives. The main results are obtained by means of the Krasnoselskii’s fixed point theorem.

2010Mathematics Subject Classification: 26A33; 93B05; 34K35

Keywords: Hyers-Ulam stability, controllability, proportional-Caputo derivatives, Krasnoselskii’s fixed point theorem

1. INTRODUCTION

Fractional differential equations have been studied extensively in the literature be- cause of their applications in various fields of engineering and science; see the books [16,18,22]. In the few past years, the variety of definitions of fractional operators has become visible to those interested in fractional calculus.Here, we focus on the most ranking kinds including Liouville, Caputo, Hadamard, Atangana-Baleanu, Caputo- Fabrizio derivatives and etc. For instance, see the books [15,23] and the papers [3,8,19–21] and the references quoted therein.

Recently, Khalil et al. [14] introduce a new definition of fractional derivative, called the conformable fractional derivative, with an obstacle that it does not tend to the original function as the orderαtends to zero. The new definition has attracted good efforts of many researchers to establish some useful results; see, for example, [5–7,17,26].

In control theory, a proportional derivative controller for controller outputuat time twith two tuning parameters has the algorithm

u(t) =κPE(t) +κd

d dtE(t),

© 2021 Miskolc University Press

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where κP andκd are the proportional control parameter and the derivative control parameter, respectively. The functionE is the error between the state variable and the process variable. This control law enables Dawei et al. [11] to present the control of complex networks models.

Inspired by the above concept of the proportional derivative controller, Anderson et al. [2] were able to define the proportional (conformable) derivative of orderαby

P

0Dtαg(t) =k1(α,t)g(t) +k0(α,t)g(t),

wheregis differentiable function andk0,k1:[0,1]×R→[0,∞)are continuous func- tions of the variabletand the parameterα∈[0,1]which satisfy the following condi- tions for allt∈R:

α→0lim+k0(α,t) =0, lim

α→1k0(α,t) =1, k0(α,t)̸=0,α∈(0,1], (1.1)

α→0lim+k1(α,t) =1, lim

α→1k1(α,t) =0, k1(α,t)̸=0,α∈[0,1). (1.2) This newly defined local derivative tends to the original function as the order α tends to zero and hence improved the conformable derivatives. In [13], Jarad et al. discussed a special case of the proportional derivatives whenk1(α,t) =1−αand k0(α,t) =α.

In [4], Baleanu et al. proposed a new more general proportional fractional derivat- ive as a linear combination of a Riemann-Liouville integral and a Caputo derivative, also they obtained some amazing results relevant to the newly hybrid fractional op- erator such as the Laplace transform and its inversion. Further, they solved some dif- ferential equations involved that new hybrid derivative and got the solution in terms of a new bivariate Mittag-Leffler function.

Inspired by the new results in [4], we investigate initial value problems for frac- tional differential equations via generalized proportional-Caputo fractional derivat- ives. Precisely, we consider the following IVP:

(PC

0 Dαt x(t) =f(t,x(t)) +Bu(t), t∈J= [0,b],b<∞,

x(0) =x0∈R, (1.3)

wherePC0 Dαt denotes the proportional-Caputo fractional derivative of orderα∈(0,1], the functionf:J×R→Ris continuous, the control functionu(·)is given inL2(J,U), a Banach space of admissible control functions withUas a Banach space, andBis a bounded linear operator fromUtoR.

Controllability is one of the fundamental notions of modern control theory, which enables one to steer the control system from an arbitrary initial state to an arbitrary final state using the set of admissible controls where initial and final state may vary over the entire space. The problem of controllability of nonlinear systems represented by fractional differential equations has been extensively studied by several authors;

see, for example, [1,9,10,25] and the references therein.

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To our knowledge there are no similar contributions to the controllability and Hyers-Ulam stability of fractional differential equations via generalized proportional- Caputo fractional derivatives.

2. PRELIMINARIES

In this section we collect some definitions, properties and propositions of the new generalized proportional-Caputo hybrid fractional derivative.

Definition 1([4]). The proportional-Caputo hybrid fractional derivative of order α∈(0,1)of a differentiable functiong(t)is given by

PC

0 Dαt g(t) = 1 Γ(1−α)

Z t 0

k1(α,τ)g(t) +k0(α,τ)g(t)

(t−τ)−αdτ, (2.1) where the function space domain is given by requiring that g is differentiable and bothgandg are locallyL1functions on the positive reals.

Definition 2([4]). The inverse operator of the proportional-Caputo hybrid frac- tional derivative of orderα∈(0,1)is given by

PC

0 Itαg(t) = Z t

0 exp

Z t

u

k1(α,s) k0(α,s)ds

RL

0 D1−αu g(u)

k0(α,u) du, (2.2) whereRL0 D1−αu denotes the Riemann-Liouville fractional derivative of order 1−αand is given by

RL

0 D1−αu g(u) = 1 Γ(α)

d du

Z u 0

(u−s)α−1g(s)ds. (2.3) For more details, we refer the reader to the book of Kilbas et al. [15].

Proposition 1([4]). The following inversion relations

PC

0 Dαt PC0 Itαg(t) =g(t)− t−α Γ(1−α)lim

t→0 RL

0 Itαg(t), (2.4)

PC

0 ItαPC0 Dαtg(t) =g(t)−exp

Z t

0

k1(α,s) k0(α,s)ds

g(0) (2.5)

are satisfied.

Proposition 2([4]). The proportional-Caputo hybrid fractional derivative oper- atorPC0 Dαt is non-local and singular.

Remark1 ([4]). In the limiting casesα→0 andα→1, we recover the following special cases:

α→0lim

PC

0 Dαt g(t) = Z t

0

g(τ)dτ,

α→1lim

PC

0 Dαt g(t) =g(t).

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Theorem 1(Krasnoselskii’s fixed point theorem, [24]). LetΩbe a closed convex and non-empty subset of a Banach spaceX. LetP1 andP2, be two operators such that

(i) P1x+P2y∈Ω, for all x,y∈Ω, (ii) P1is compact and continuous, (iii) P2is a contraction mapping.

Then there exists z∈Ωsuch that z=P1z+P2z.

3. CONTROLLABILITYRESULTS

In this section, we employ the generalized proportional Caputo fractional derivat- ive operator to discuss the controllability of the IVP (1.3).

LetC(J,R) be the Banach space of all real-valued continuous functions from J intoRequipped by the norm∥x∥=supt∈[0,T]|x(t)|.

Firstly, we consider the following auxiliary lemma.

Lemma 1. Let 0<α≤1 and h∈C(J,R). Then the solution of the following linear fractional differential equation

(PC

0 Dtαx(t) =h(t), t∈J,

x(0) =x0, (3.1)

is equivalent to the Volterra integral equation x(t) =exp

Z t

0

k1(α,s) k0(α,s)ds

x0

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) h(τ)dτdu. (3.2) Proof. Applying the operatorPC0 Itα(·)on both sides of (3.1), we get

PC

0 ItαPC0 Dαtx(t) =PC0 Itαh(t).

Using (2.2) and (2.3) together with Proposition1, we get x(t)−exp

Z t

0

k1(α,s) k0(α,s)ds

x(0) =

Z t 0

exp

Z t

u

k1(α,s) k0(α,s)ds

RL

0 D1−αu h(u) k0(α,u) du.

In view of the following elementary fact:

RL

0 D1−αu h(u) =RL0 Iu−(1−α)h(u) =RL0 Iuα−1h(u) = 1 Γ(α−1)

Z u 0

(u−τ)α−2h(τ)dτ, one can easily obtain the desired integral equation (3.3). The converse follows by

direct computation. This completes the proof. □

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By virtue of Lemma1, the solution of the IVP (1.3) is given by x(t) =exp

Z t

0

k1(α,s) k0(α,s)ds

x0

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) f(τ,x(τ))dτdu

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) Bux(τ)dτdu. (3.3) The following definition is helpful in the discussion of the controllability of the IVP (1.3).

Definition 3. The IVP (1.3) is said to be controllable on the intervalJif, for every x0,x1∈R, there exists a controlu∈L2(J,U)such that a solutionxof equation (1.3) satisfiesx(b) =x1.

The following assumptions will be imposed.

(A1) The function f :J×R→Ris continuous.

(A2) There exists a constantL>0 such that

|f(t,x)−f(t,y)| ≤L|x−y|, for all t∈J, x,y∈R. (A3) The linear operatorW:L2(J,U)→R, defined by

Wu= 1

Γ(α−1) Z b

0

Z u 0

exp

Z b

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) Bu(τ)dτdu has an induced inverse operatorW−1 which takes values inL2(J,U)/kerW, where the kernel space ofWis defined by kerW={x∈L2(J,U):Wx=0} and there exist constantsM1,M2>0 such that∥B∥ ≤M1and∥W−1∥ ≤M2. Now we formulate the first main theorem of the paper.

Theorem 2. If the assumptions(A1)−(A3) are satisfied. Then the IVP (1.3) is controllable on J, provided that

M1M2bL

M2kΓ2(α+1) <1, (3.4)

whereinft∈J|k0(α,t)|=Mk̸=0.

Proof. Set supt∈J|f(t,0)|=Mf <∞.

We consider the setBr={x∈C(J,R):∥x∥ ≤r)}withr≥ Λ1 1−Λ2

.

For the purpose of expediency, we define the two constantsΛ1>0 and 0<Λ2<1 as

Λ1=|x0|+ Mfbα

MkΓ(α+1)+ M1M2bα MkΓ(α+1)

h

|x1|+|x0|+ Mfbα MkΓ(α+1)

i ,

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Λ2= Lbα MkΓ(α+1)

1+ M1M2bα MkΓ(α+1)

.

Define the controlux(t)by ux(t) =W−1h

x1exp

Z b

0

k1(α,s) k0(α,s)ds

x0

+ 1

Γ(α1) Z b

0 Zu

0

exp

Zb

u

k1(α,s) k0(α,s)ds

(uτ)α−2

k0(α,u) f(τ,x(τ))dui

(t),tJ.

Later, we shall use the following estimates:

∥ux=sup

t∈J

|ux(t)|

M2sup

t∈J

n|x1|+|x0|+ 1 Γ(α1)

Zb 0

Z u 0

(uτ)α−2

|k0(α,u)| |(f(τ,x(τ))−f(τ,0)) +f(τ,0)|dτduo

M2sup

t∈J

n|x1|+|x0|+ 1 Γ(α1)

Zb 0

Z u 0

(uτ)α−2

|k0(α,u)| |f(τ,x(τ))−f(τ,0)|+|f(τ,0)|

duo

M2sup

t∈J

n|x1|+|x0|+ 1 Γ(α1)

Zb 0

Z u 0

(uτ)α−2

|k0(α,u)| L|x(τ)|+|f(τ,0)|

duo

M2h

|x1|+|x0|+ bα

MkΓ(α+1) L∥x∥+Mfi

, (3.5)

and

∥ux−uy∥=sup

t∈J

|ux(t)−uy(t)|

≤M2sup

t∈J

( 1 Γ(α−1)

Z b 0

Z u 0

(u−τ)α−2

|k0(α,u)| |f(τ,x(τ))−f(τ,y(τ))|dτdu )

≤ M2L

MkΓ(α−1)sup

t∈J

( Z b

0

Z u 0

(u−τ)α−2|x(τ)−y(τ)|dτdu )

≤ M2Lbα

MkΓ(α+1)∥x−y∥. (3.6)

Using the controlux(t), we define the operatorsP1,P2onBras:

(P1x)(t) =exp

Z t

0

k1(α,s) k0(α,s)ds

x0

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) f(τ,x(τ))dτdu, (P2x)(t) = 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) Bux(τ)dτdu.

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Clearly, one can notice that(P1x+P2x)(b) =x1. This means thatux steers the IVP (1.3) fromx0tox1in finite timeb, which implies that the IVP (1.3) is controllable on J.

The proof is divided into three main steps.

Step 1.P1x+P2y∈Br, ∀x,y∈Br.

For eacht∈Jandx,y∈Br, using (3.5), one has

P1x+P2y∥=sup

t∈J

|(P1x)(t) + (P2y)(t)|

sup

t∈J

( exp

Zt

0

k1(α,s) k0(α,s)ds

|x0|

+ 1

Γ(α1) Z b

0 Z u

0

exp

Z t

u

k1(α,s) k0(α,s)ds

× (uτ)α−2

|k0(α,u)| |(f(τ,x(τ))f(τ,0)) +f(τ,0)|du

+ 1

Γ(α1) Z b

0 Z u

0

exp

Z t

u

k1(α,s) k0(α,s)ds

(uτ)α−2

|k0(α,u)| |Buy(τ)|du )

≤ |x0|+ 1 MkΓ(α1)

Z b 0

Z u 0

(uτ)α−2 L∥x∥+Mf du

+ 1

MkΓ(α1) Z b

0 Z u

0

(uτ)α−2∥B∥∥uydu

≤ |x0|+ bα

MkΓ(α+1) Lr+Mf + M1M2bα

MkΓ(α+1)

h|x1|+|x0|+ bα

MkΓ(α+1) Lr+Mfi

≤ |x0|+ Mfbα

MkΓ(α+1)+ M1M2bα MkΓ(α+1)

h|x1|+|x0|+ Mfbα MkΓ(α+1)

i

+ Lbα MkΓ(α+1)

1+ M1M2bα MkΓ(α+1)

r

=Λ1+Λ2rr.

Thus, we conclude thatP1x+P2y∈Br.

Step 2.P1is compact and continuous. Firstly, we show thatP1is continuous. Let {xn}be a sequence such thatxn→xasn→∞inBr. Thus, for eacht∈J, we have

∥P1xn−P1x∥=sup

t∈J

|(P1xn)(t)−(P1x)(t)|

≤ 1

MkΓ(α−1) Z t

0

Z u 0

(u−τ)α−2∥(f(·,xn(·))−f(·,x(·))∥dτdu.

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Therefore, the continuity of f implies thatP1is continuous.

Next, we show thatP1is uniformly bounded onBr. For eachtJandxBr, one has

∥P1x∥=sup

t∈J

|(P1x)(t)|

≤sup

t∈J

( exp

Z t

0

k1(α,s) k0(α,s)ds

|x0|+ 1 Γ(α−1)

Z b 0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

×(u−τ)α−2

|k0(α,u)||(f(τ,x(τ))−f(τ,0)) +f(τ,0)|dτdu )

≤ |x0|+ bα

MkΓ(α+1) Lr+Mf ,

which implies thatP1is uniformly bounded onBr.

It remains to show thatP1is equicontinuous. For eacht1,t2∈J,t1<t2andx∈Br, one obtain that:

∥(P1x)(t2)(P1x)(t1)∥

exp Z t2

0

k1(α,s) k0(α,s)ds

!

x0exp Zt1

0

k1(α,s) k0(α,s)ds

! x0

+ 1

Γ(α1)

Zt2 0

Z u 0

"

exp Zt2

0

k1(α,s) k0(α,s)ds

!

exp Z t1

0

k1(α,s) k0(α,s)ds

!#

×(uτ)α−2

k0(α,u) (f(τ,x(τ))du

+ 1

Γ(α1)

Zt2 t1

Z u 0

exp Z t1

0

k1(α,s) k0(α,s)ds

!(uτ)α−2

k0(α,u) (f(τ,x(τ))dτdu

=

k1(α,ξ)

k0(α,ξ)x0exp Z ξ

0

k1(α,s) k0(α,s)ds

! (t2t1)

+ 1

Γ(α1)

Zt2 0

Z u 0

k1(α,ξ)

k0(α,ξ)exp Z ξ

0

k1(α,s) k0(α,s)ds

!

(t2t1)(uτ)α−2

k0(α,u) (f(τ,x(τ))dτdu

+ 1

Γ(α1)

Zt2 t1

Z u 0

exp Z t1

0

k1(α,s) k0(α,s)ds

!(uτ)α−2

k0(α,u) (f(τ,x(τ))dτdu

k1(α,ξ) k0(α,ξ)x0

(t2−t1) + f¯ Γ(α+1)

k1(α,ξ) k20(α,ξ)

t2(t2−t1) + f¯ Γ(α+1)

1 k0(α,ξ)

(t2αt1α),

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where ¯f =supt∈J×Br|f(t,x(t)| andξ∈(t1,t2). Ast1 →t2, the right hand side of the above inequality tends to zero independently ofx∈Br. As a consequence of the Arzel`a-Ascoli theorem, we deduce thatP1is compact onBr.

Step 3.P2is a contraction onBr.

For eacht∈Jandx,y∈Br, using (3.6), one has

P2xP2y∥=sup

t∈J

|(P2x)(t)−(P2y)(t)|

=sup

t∈J

( 1 Γ(α1)

Zt 0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(uτ)α−2

k0(α,u) B(ux(τ)uy(τ))du )

M1bα

MkΓ(α+1)∥ux−uy

M1M2bL

Mk2Γ2+1)∥x−y∥.

In view of the condition (3.4), we conclude thatP2is a contraction mapping.

Therefore, all the assumptions of Krasnoselskii’s fixed point theorem (Theorem1) are satisfied. Hence, the IVP (1.3) is controllable onJ. This completes the proof. □

4. HYERS-ULAMSTABILITY

Here, we elucidate Hyers-Ulam stability of the IVP (1.3). We begin with the following essential definition.

Definition 4([12]). The integral equation (3.3) is said to be Hyers-Ulam stable, if there exists a constantµ>0 satisfying: for everyε>0, if

x(t)−exp

Z t

0

k1(α,s) k0(α,s)ds

x0

− 1 Γ(α−1)

Z t 0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) f(τ,x(τ))dτdu

− 1 Γ(α−1)

Z t 0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) Bux(τ)dτdu

≤ε, there exists a continuous functionx(t)satisfying

x(t) =exp

Z t

0

k1(α,s) k0(α,s)ds

x0

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) f(τ,x(τ))dτdu

+ 1

Γ(α−1) Z t

0

Z u 0

exp

Z t

u

k1(α,s) k0(α,s)ds

(u−τ)α−2

k0(α,u) Bux(τ)dτdu, (4.1)

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such that

|x(t)−x(t)| ≤µε, ∀t∈J.

Theorem 3. Assume that the assumptions(A1)−(A3)are satisfied. Then the IVP (1.3) is Hyers-Ulam stable.

Proof. With the help of Theorem2, letx(t)be unique solution of (3.3) andx(t) be any other solution satisfying (4.1). Then, by a similar way in the proof of Theorem 2and by virtue of (3.6), one has

|x(t)−x(t)| ≤ 1 MkΓ(α−1)

Z t 0

Z u 0

(u−τ)α−2|f(τ,x(τ))−f(τ,x(τ))| dτdu

+ M1

MkΓ(α−1) Z t

0

Z u 0

(u−τ)α−2|ux(τ)−ux(τ)|dτdu

≤ L

MkΓ(α−1) Z t

0

Z u 0

(u−τ)α−2|x(τ)−x(τ)|dτdu

+ M1

MkΓ(α−1) Z t

0

Z u 0

(u−τ)α−2|ux(τ)−ux(τ)|dτdu

bαL

MkΓ(α+1)+ M1M2bL Mk2Γ2(α+1)

∥x−x

=µ∥x−x∥, where

µ:= bαL

MkΓ(α+1)+ M1M2bL M2kΓ2(α+1).

Therefore, the integral equation (3.3) is Hyers-Ulam stable. Consequently, the IVP

(1.3) is Hyers-Ulam stable. The proof is finished. □

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Author’s address

Mohamed I. Abbas

Alexandria University, Faculty of Science, Department of Mathematics and Computer Science, Al- exandria, 21511, Egypt

E-mail address:miabbas@alexu.edu.eg; miabbas77@gmail.com

Hivatkozások

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