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R E S E A R C H

Open Access

Fractional optimal control problem for

differential system with delay argument

G. Mohamed Bahaa

*

*Correspondence:

[email protected] Present address: Department of Mathematics, Dean of Academic Services, Taibah University, Al-Madinah Al-Munawarah, Saudi Arabia

Permanent address: Department of Mathematics, Faculty of Science, Beni-Suef University, Beni-Suef, Egypt

Abstract

In this paper, we apply the classical control theory to a fractional differential system in a bounded domain. The fractional optimal control problem (FOCP) for differential system with time delay is considered. The fractional time derivative is considered in a Riemann-Liouville sense. We first study the existence and the uniqueness of the solution of the fractional differential system with time delay in a Hilbert space. Then we show that the considered optimal control problem has a unique solution. The performance index of a FOCP is considered as a function of both state and control variables, and the dynamic constraints are expressed by a partial fractional differential equation. The time horizon is fixed. Finally, we impose some constraints on the boundary control. Interpreting the Euler-Lagrange first order optimality condition with an adjoint problem defined by means of a right fractional Caputo derivative, we obtain an optimality system for the optimal control. Some examples are analyzed in detail.

MSC: 46C05; 49J20; 93C20

Keywords: fractional optimal control problems; fractional differential systems; time delay; Dirichlet and Neumann conditions; existence and uniqueness of solutions; Riemann-Liouville sense; Caputo derivative

1 Introduction

An optimal control problem (OCP) deals with the problem of finding a control law for a given dynamic system that minimizes a performance index in terms of the state and con-trol variables. Various optimization problems associated with the integer optimal concon-trol of differential systems with time delays were studied recently by many authors; see for in-stance [–] and the references therein). For example in [] Bahaa found the optimality conditions for cooperative parabolic systems governed by a Schrödinger operator.

The OCP reduces to a fractional optimal control problem (FOCP) when either the per-formance index or the dynamic constraints or both include at least one fractional-order derivative term. The theory of fractional differential equations has received much atten-tion over the past  years, since they are important in describing the natural models such as in diffusion processes, stochastic processes, finance, and hydrology. However, the number of publications on fractional optimal control problem (FOCPs) has grown; see for example [–] and the references therein). For example in [], Agrawal presented a gen-eral formulation and solution scheme for fractional optimal control problem. That is, an

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optimal control problem in which either the performance index or the differential equa-tions governing the dynamics of the system or both contain at least one fractional deriva-tive term. In that paper, the fractional derivaderiva-tive was defined in the Riemann-Liouville sense and the formulation was obtained by means of fractional variation principle and the Lagrange multiplier technique. Following the same technique, Fredericoet al.[] ob-tained a Noether-like theorem for fractional optimal control problem in the sense of Ca-puto. Recently, Agrawal [] presented an eigenfunction expansion approach for a class of distributed system whose dynamics is defined in the sense of Caputo. In [], Bahaa studied the fractional optimal control problem for variational inequalities with control constraints. In [], Bahaa studied the fractional optimal control problem for differential systems with control constraints involving second order operator and in [] involving infinite order operator.

Additionally, if the dynamic constraints or the performance index contain delay argu-ments, we are faced with a delay fractional optimal control problem (DFOCP). A strong motivation for studying and investigating the solution and the properties for fractional differential equations with time delay comes from the fact that they describe efficiently anomalous diffusion on fractals (physical objects of fractional dimension, like some amor-phous semiconductors or strongly porous materials, fractional random walk, etc. Other applications occur in the following fields: fluid flow, viscoelasticity, control theory of dy-namical systems, diffusive transport akin to diffusion, electrical networks, probability and statistics, dynamical processes in self-similar and porous structures, electrochemistry of corrosion, optics and signal processing, rheology, etc.

However, the existence of delay in the dynamic system may cause difficulty in the con-trol and analysis of such systems. Therefore, constructing new analytical and numerical techniques for the delay fractional dynamic systems has become a strong topic to be con-sidered; see [–] and the references therein. For instance in [] an efficient linear pro-gramming formulation is proposed for a class of fractional-order optimal control problems with delay argument. By means of the Lagrange multiplier in the calculus of variations and using the formula for fractional integration by parts, the Euler-Lagrange equations are de-rived in terms of a two-point fractional boundary value problem including an advance term as well as the delay argument. In [, ], Jarad studied the fractional variational op-timal control problems with delay argument. Various fractional opop-timal control problems are also studied by Mophouet al.when the fractional time derivative is expressed in the Riemann-Liouville sense. For instance, we refer to the boundary optimal control [] and the optimal control of a fractional diffusion equation with state constraints []. In [] Mophou was concerned with the optimal control of the fractional diffusion equation with delay with Caputo fractional derivatives. However, the DFOCP is an issue that still needs to be investigated as proved by the poor literature on the topic.

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analysis we can characterize the optimal control of a system of partial differential equa-tions and inequalities, which can be applied to concrete fractional diffusion equaequa-tions.

This paper is organized as follows. In Section , we introduce some definitions and pre-liminary results. In Section , we formulate the fractional Dirichlet problem. In Section , we show that our fractional optimal control problem holds and we give the optimality system for the optimal control. In Section , we formulate the fractional Neumann prob-lem. In Section , the minimization problem is formulated and we state some illustrative examples. In Section , we state our conclusion of the paper.

2 Some basic definitions

In this section, we state some definitions and results which will be used later.

LetnN∗andbe a bounded open subset ofRnwith a smooth boundaryof class C. For a timeT> , we setQ=×(,T) and=×(,T).

The following definitions and remarks can be found in the literature (see [, , , ]).

Definition . Letf :R+→Rbe a continuous function onR+andβ> . Then the ex-pression

I+βf(t) =  (β)

t

(ts)β–f(s)ds, t> ,

is called the Riemann-Liouville integral of orderβ, where(·) is the Gamma function defined for any complex numberzby

(z) = 

t

z–etdt.

Definition . Letf:R+→R. The Riemann-Liouville fractional derivative of orderβof

f is defined by

+f(t) =  (nβ)

dn dtn

t

(ts)nβ–f(s)ds, t> ,

whereβ∈(n– ,n),nN. Whenβ is an integer the left derivative is replaced byD, the ordinary differential operator.

Definition . Letf :R+→R. The left Caputo fractional derivative of orderβ off is defined by

f(t) =  (nβ)

t

(ts)nβ–f(n)(s)ds, t> ,

whereβ∈(n– ,n),nN.

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Lemma . Let T> ,uCm([,T]),p(m– ,m),mN and vC([,T]).Then for

Remark .f(t) is the so-called right fractional Caputo derivative. It represent the

future state off(t). For more details on the derivative we refer to [, , , ]. Note also

We also introduce the space

W(,T) :=y;yL,T;H(),+y(t)∈L,T;H–()

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3 Fractional Dirichlet problem for differential equations with time lags

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Proof differentiable in ],T[ and the bilinear form (.) is symmetric,

π(t;y,φ) =π(t;φ,y) ∀y,φH(). (.)

The system of equations (.)-(.) defines our fractional problem with time delay. By using the Lax-Milgram lemma, we can study the existence of a unique solution of the

fractional system (.)-(.).

Lemma .(see [, , , ] (fractional Green’s formula)) Let y be the solution of system

(.)-(.).Then we have,for anyφC∞(Q)so thatφ(x,T) = inandφ= on,

Lemma . We can state equations(.)-(.)in a more convenient form,first let us define the operatorMby

Then equations(.)-(.)have the following form:

+y(x,t) +A(t)y(x,t) +My(x,t) =f, x,t∈(,T), (.)

y(x, ) =g(x, ), x, (.)

I+–βyx, +=y(x), x, (.)

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We can notice that equations(.)and(.)are equivalent in(,T).But in the interval

(,ω)from equations(.)-(.)we get

+y(x,t) +A(t)y(x,t) =+g(x,t) +A(t)g(x,t), x,t∈(,ω), (.)

y(x, ) =g(x, ), x,t= , (.)

Lemma . By using(Theorem.,Lions),we can easily show that yg in(,ω).

By using a constructive method we can prove the existence and uniqueness of the solution of equations(.)-(.).Firstly,we solve(.)-(.)in the subinterval(,ω)and then in the subinterval(ω, ω)etc.,until the procedure covers the whole interval(,T).In this way the solution in the previous step determines the next one.In fact,in every subinterval the solution of equations(.)-(.)exists and is unique(Theorem.,Ref. []).If the right-hand sides of equations(.)-(.)are equal to zero,then there exists only a trivial solution of equations(.)-(.),i.e.,y≡.

A more general case (e.g., whenωis a function of the timet) can be treated analogously as in Ref. [] see Lemma ..

Lemma . If(.), (.)holds,then the system(.)-(.)has a unique solution yW(,T).

Proof By using the coerciveness condition (.) and the Lax-Milgram theorem, there ex-ists a unique solutiony(t)∈H

which is equivalent to the existence of a unique solutiony(t)∈H () for

which can be written as

This is known as the variational fractional Dirichlet problem, whereL(φ) is a continuous linear form onH

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that is, the PDE

Let us multiply both sides in (.) byφand applying Green’s formula (Lemma .), we have

whence comparing with (.), (.)

Lemma . We can extend our fractional problem(.)-(.)to a more general situation as follows.Let

4 Optimization theorem and the fractional control problem

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The observation equation is given by

z(u) =y(u), (.)

The cost functionJ(v) is given by

J(v) =

Q

y(v) –zddx dt+ (Nv,v)L(Q), (.)

wherezdis a given element inL() andNL(L(Q),L(Q)) is a hermitian positive defi-nite operator:

(Nu,u)≥cuL(Q), c> . (.)

Control constraints:We defineUad(the set of admissible controls) to be a closed, convex

subset ofU=L(Q).

Control problem:We want to minimizeJoverUadi.e.findusuch that

J(u) = inf vUad

J(v). (.)

Under the given considerations we have the following theorem.

Theorem . The problem(.)admits a unique solution given by(.)-(.)and by

Q

p(u) +Nu(vu)dx dt≥, (.)

where p(u)is the adjoint state.

Proof Since the controluUadis optimal if and only if

J(u)(vu)≥ for allvUad.

The above condition, when explicitly calculated for this case, gives

y(u) –zd,y(v) –y(u)L(Q)+ (Nu,vu)L(Q)≥

i.e.

Q

y(u) –zdy(v) –y(u)dx dt+ (Nu,vu)L(Q)≥. (.)

For the controluL(Q) the adjoint statep(u)L(Q) is defined by

Dβp(u) +A∗(t)p(u) +Mp(u) =y(u) –zd, inQ, (.)

p(u) = , on, (.)

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Now, multiplying equation (.) by (y(v) –y(u)) and applying Green’s formula, we obtain

and hence (.) is equivalent to

which completes the proof.

Example . In the case of no constraints on the control (Uad=U), then (.) reduces to

p+Nu=  on.

The fractional optimal control is obtained by the simultaneous solution of the following system of fractional partial differential equations:

+y+A(t)y+My=f, –Dβp+A∗(t)p+Mp=yzd inQ,

y+N–p|= , p=  on,

I+–βy(x, ) =y(x), p(x,T) = , x,

further

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Example . Take

Uad=u|uL(),u≥ almost everywhere on.

The optimal control is obtained by the solution of the fractional problem

+y+A(t)y+My=f, –Dβp+A∗(t)p+Mp=yzd inQ,

y≥, p=  on,

p+Ny≥, [p+Np] =  on,

I+–βy(x, ) =y(x), p(x,T) = , x,

hence

u=y|.

Example . We consider the fractional diffusion equation with Caputo fractional deriva-tives and time delay. We have

y(t) –y(t) +My=v, t∈[,T], (.)

y() =y, x, (.)

y(x,t) = , x,t∈(,T), (.)

wherey∈H()∩H(),is the Laplace operator and the controlvbelongs toL(Q). We can minimize

J(v) =y(v) –zd

L(Q)+NvL(Q), zdL(Q),N> , (.)

subject to system (.)-(.) and the optimal controlvwill be characterized by system (.)-(.) with the adjoint system

p(t) –p(t) +My=yz

d, t∈[,T], (.)

p(x,t) = , x,t∈(,T), (.)

p(x,T) = , x, (.)

and with the optimality condition

v= –p

N inQ. (.)

Example . We can also consider the fractional diffusion equation with Riemann-Liouville fractional derivatives and time delay:

+y(t) –y(t) +My=v, t∈[,T], (.)

IT–β(t)y

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y(x,t) = , x,t∈(,T), (.)

whereIT–β(t)y(+) =limt→+I–β(t)

T y(t), the controlvbelongs toL(Q). We can minimize

the cost function (.) subject to system (.)-(.) and the optimal controlvwill be characterized by system (.)-(.) with the adjoint system (.)-(.) and with the optimality condition (.).

5 Fractional Neumann problem for differential system with time delay

SinceH()⊂H() we can show that the bilinear form (.) is coercive inH(), that is,

π(y,y)≥cyH(), c>  for allyH(). (.)

Also we have the following.

Lemma . If(.)holds,then there exists a unique solution yH()such that

+y+A(t)y+My=f in Q, (.)

∂y

∂νA(t)

=h on, (.)

I+–βy+=y(x), x, (.)

where

∂y

∂νA(t) =

n

i,j=

aij

∂y

∂xjcos(n,xj) on,

cos(n,xj)is the ith direction cosine of n,n being the normal atexterior to.

Proof By using the coerciveness condition (.) and the Lax-Milgram lemma, there exists a unique solutionyH() so that

Q

yDβψ+Aψ+Mψdx dt=M(ψ) for allψH(). (.)

This is known as the fractional Neumann problem, whereM(ψ) is a continuous linear form onH() taking the form

M(ψ) =

Q

fψdx dt+

yψ(x, )dx

h ∂ψ

∂νA

d, (.)

fL(Q),y∈L(),hH().

Equation (.) is equivalent to

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Let us multiply both sides in (.) byψand by using Green’s formula, we get

whence comparing with (.), (.)

6 Fractional minimization theorem and boundary control problem

We consider the spaceU=L() (the space of controls), for every controluU, the state

For the observation, we consider the following two cases:

(i)

z(u) =y(u). (.)

(ii) Observation of the final state

z(u) =y(x,T;u). (.)

Case (i): The cost function is given by

J(v) =

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Control problem:We wish to find

inf vUad

J(v). (.)

Under the given considerations we have the following theorem.

Theorem . Assume that(.)holds and the cost function is given by(.).The optimal control u is characterized by(.), (.), (.)together with

Dβp(u) +A∗(t)p(u) +Mp(u) =y(u) –zd in Q, (.) ∂p(u)

∂νA∗ =  on, (.)

p(x,T;u) = , x, (.)

and the optimality condition is

p(u) +Nu(vu)d≥ ∀vUad, (.)

where p(u)is the adjoint state.

Proof The controluUadis optimal if and only if

J(u)(vu)≥ ∀vUad, (.)

that is,

y(u) –zd,y(v) –y(u)L(Q)+ (Nu,vu)U≥. (.)

The adjoint state is given by the solution of the adjoint Neumann problem (.), (.), (.). Multiplying equation (.) byy(v) –y(u) and by using Green’s formula, having in mind the conditions in (.), (.), we obtain

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Hence we substituted from (.) in (.), to get

p(u)(vu)d+ (Nu,vu)L()≥,

i.e.

p(u) +Nu(vu)d≥ ∀vUad,

which completes the proof.

Example . In the case of no constraints on the control (Uad=U), then (.) reduces to

p+Nu=  on.

The fractional optimal control is obtained by the simultaneous solution of the following system of fractional partial differential equations:

+y+A(t)y+My=f, –Dβp+A∗(t)p+Mp=yzd inQ,

∂y

∂νA

+N–p|= ,

∂p

∂νA

=  on,

I+–βy(x, ) =y(x), p(x,T) = , x,

further

u= –N–(P|).

Example . Take

Uad=u|uL(),u≥ almost everywhere on.

The optimal control is obtained by the solution of the fractional problem

+y+A(t)y+My=f, –Dβp+A∗(t)p+Mp=yzd inQ, ∂y

∂νA≥,

∂p

∂νA∗ =  on,

p+N ∂y

∂νA≥,

∂y

∂νA

p+N ∂y

∂νA

=  on,

I+–βy(x, ) =y(x), p(x,T) = , x,

hence

u= ∂y ∂νA

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Case (ii): Observation of the final state

z(u) =y(x,T;u).

The cost function is given by

J(v) =

y(x,T;v) –zd

dx+ (Nv,v)L(), zdL().

The adjoint state is defined by

Dβp(u) +A∗(t)p(u) +Mp(u) =  inQ, ∂p(u)

∂νA∗ = , on,

p(x,T;u) =y(x,T;u) –zd(x), x,

and the optimality condition is

(p+Nu)(vu)d≥ ∀vUad, (.)

wherep(u) is the adjoint state.

Example . In the case of no constraints on the control (Uad=U), then (.) reduces to

p+Nu=  on.

The optimal control is obtained by the simultaneous solution of the following system of fractional partial differential equations:

+y+A(t)y+My=f, –Dβp+A∗(t)p+Mp=  inQ,

∂y

∂νA

+N–p|

= ,

∂p

∂νA∗ =  on,

I+–βy(x, ) =y(x), p(x,T) =y(x,T;u) –zd(x), x,

further

u= –N–(P|).

Example . If we take

Uad=u|uL(),u≥ almost everywhere on,

then (.) is equivalent to

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Example . We consider the Neumann fractional diffusion equation with Caputo frac-tional derivatives and time delay,

y(t) –y(t) +My=v, t∈[,T], (.)

y() =y, x, (.)

∂y(x,t)

∂νA = , x,t∈(,T), (.)

wherey∈H()∩H(),is the Laplace operator and the controlvbelongs toL(Q). We can minimize

J(v) =y(v) –zd

L(Q)+NvL(Q), zdL(Q),N> , (.)

subject to system (.)-(.) and the optimal controlvwill be characterized by system (.)-(.) with the adjoint system

p(t) –p(t) +My=yz

d, t∈[,T], (.)

∂p(x,t)

∂νA∗ = , x,t∈(,T), (.)

p(x,T) = , x, (.)

and with the optimality condition

v= –p

N inQ. (.)

Example . We can also consider the Neumann fractional diffusion equation with Riemann-Liouville fractional derivatives and time delay:

+y(t) –y(t) +My=v, t∈[,T], (.)

I–

β(t)

T y

+=y, x, (.)

∂y(x,t)

∂νA = , x,t∈(,T), (.)

whereI–

β(t)

T y(+) =limt→+I–β(t)

T y(t), the controlvbelongs toL(Q). We can minimize

the cost function (.) subject to system (.)-(.) and the optimal controlvwill be characterized by system (.)-(.) with the adjoint system (.)-(.) and with the optimality condition (.).

Remark . If we takeβ=  in the previous sections we obtain the classical results in the optimal control with integer derivatives.

7 Conclusions

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optimal control problems. The formulation presented and the resulting equations are very similar to those for classical optimal control problems. The optimization problem presented in this paper constitutes a generalization of the optimal control problem of parabolic systems with Dirichlet and Neumann boundary conditions, considered by Lions

et al.[, ], Podlubny [], Oldhamet al.[], Bahaaet al.[–, –] and Kotarskiet al.[, –], to the fractional optimal control problem for second order systems with time delay.

Competing interests

The author declares that he has no competing interests.

Acknowledgements

The author would like to express his gratitude to the anonymous reviewers for their very valuable remarks and comments.

Received: 30 September 2016 Accepted: 21 February 2017 References

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