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Time optimal controls for fractional differential systems with Riemann-Liouville derivatives

  • TingTing Lian EMAIL logo , ZhenBin Fan and Gang Li
Published/Copyright: February 9, 2019

Abstract

Time optimal control problems governed by Riemann-Liouville fractional differential system are considered in this paper. Firstly, the existence results are obtained by using the theory of semigroup and Schauder’s fixed point. Secondly, the new approach of establishing time minimizing sequences twice is applied to acquire the time optimal pairs without the Lipschitz continuity of nonlinear function. Moreover, the reflexivity of state space is removed with the help of compact method. Finally, an example is given to illustrate the main conclusions. Our work essentially improves and generalizes the corresponding results in the existing literature.

1 Introduction

In the last dozen years or so, fractional differential equations have been served as mathematical models for describing various phenomena in the field of physics, biology, engineering, etc. For more details, we refer to the books [12, 15, 24], the recent papers [1, 2, 3, 4, 7, 13, 17, 21, 27, 28, 34] and the reference therein. The advantages of fractional derivatives over integer derivatives are the memory and genetic properties. On the other hand, Heymans and Podlubny [8] indicated that the initial conditions of differential systems with Riemann-Liouville fractional derivative are more accordant with practical circumstances in the field of viscoelasticity than that with Caputo fractional derivative. So, lot’s of scholars have done much research in this area, see [5, 16, 18, 19, 20, 23, 30] and the references therein. Fan [5], Li and Peng [16] and Mei et al. [23] investigated the Riemann-Liouville fractional differential systems by using the theory of fractional resolvent. Liu and Li [18] established the sufficient conditions for the approximate controllability of Riemann-Liouville fractional differential systems by the iterative and approximate method.

Time optimal control is a classical and important topic in the theory of optimal controls for both finite and infinite dimensional systems. To our knowledge, the time optimal pairs have been derived provided that the nonlinear function is Lipschitz continuous and both the state space X and the control space Y are reflexive (see e.g. [10, 11, 14, 26, 29, 32]). The Lipschitz continuity guarantees the existence and uniqueness of mild solution of the corresponding differential systems, and the reflexivity of the spaces X and Y ensure the weak convergence of solution sequences and control sequences, respectively.

Inspired by the above mentioned papers, it is our intension to deal with the time optimal control problems subjected to the following differential system with the Riemann-Liouville fractional derivative:

{LDγy(t)=Ay(t)+g(t,y(t))+B(t)u(t),t(0,c],I1γy(t)|t=0=y0X,uUad,(1.1)

where 0 < γ < 1, y(t) ∈ X and u(t) ∈ Y. The linear operator A : D(A) ⊆ XX generates a C0 semigroup {T(t)}t ≥ 0. BL([0, c], 𝓛(Y, X)). The admissible set Uad for control functions and the nonlinear function g : [0, c] × XX will be given in Section 2. The following two improvements are made in this article. One is that the Lipschitz continuity of g is removed without imposing any other conditions, and the solvability of (1.1) is acquired in a new space C1−γ([0, c], X) using the theory of semigroup. Inspired by Zhu and Huang [35], the new idea of setting up time minimizing sequences twice is used to compensate the lack of uniqueness of mild solutions. The other is that the reflexivity of X is no longer required by making full use of the compact method. So, our work essentially improves some related results on this topic.

This paper is structured as follows. Section 2 presents the preliminaries and basic assumptions for system (1.1). We establish the solvability of system (1.1) in Section 3. Section 4 solves the time optimal control problems subjected to system (1.1). An example is proposed to illustrate our main results in Section 5.

2 Preliminaries and Basic Assumptions

Throughout this paper, let X be a Banach space and Y be a separable reflexive Banach space. ℝ and ℝ+ are the sets of real numbers and nonnegative real numbers, respectively. The set of all continuous functions from [0, c] to Banach space X with ∥yC = sup{∥y(t)∥, t ∈ [0, c]} is denoted by C([0, c], X), and the Banach space C1−γ([0, c], X) = {y : ⋅1−γy(⋅) ∈ C([0, c], X), 0 < γ < 1} with ∥yC1−γ = sup{∥t1−γy(t)∥, t ∈ [0, c]}, where t1γy(t)|t=0=limt0+t1γy(t). We also denote by Lp ([0, c], X) the space of Bochner integrable functions from [0, c] to Banach space X with fLp=(0cf(t)pdt)1/p, where 1 ≤ p < ∞. Let L ([0, c], X) be the set of all essentially bounded functions on [0, c] with values in X and ∥f = esssup{∥f(t)∥, t ∈ [0, c]}, and 𝓛(X, Y) be the space of all linear and continuous operators from X to Y with the operator norm ∥⋅∥. 𝓛(X) represents the space 𝓛(X, X) especially.

Let f : [0, ∞) → X be an appropriate abstract function. The Riemann-Liouville fractional integral and fractional derivative of order 0 < γ < 1 are defined by

Iγf(t)=0tgγ(tτ)f(τ)dτ,

and

LDγf(t)=ddt0tg1γ(tτ)f(τ)dτ,

respectively, provided the right sides exist, where gγ(t):=tγ1Γ(γ),t>0.

Now, we give the mild solution of system (1.1) in the space C1−γ([0, c], X) using the Laplace transformation, some proper density function as well as the definition of Riemann-Liouville fractional derivatives. For details, see the recent paper [18].

Definition 2.1

A function yC1−γ([0, c], X) is called the mild solution of (1.1) if

y(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,y(τ))+B(τ)u(τ)]dτ,

for each t ∈ (0, c] and uUad, where

Sγ(t)=γ0θhγ(θ)T(tγθ)dθ,
hγ(θ)=1γθ11γωγ(θ1γ)0,θ(0,),
ωγ(θ)=1πn=1(1)n1θnγ1Γ(nγ+1)n!sin(πnγ),θ(0,).

Remark 2.1

The function ωγ(⋅) is an one-side stable probability density defined on (0, ∞) (see [22]), whose Laplace transformation satisfies

0eλθωγ(θ)dθ=eλγ,γ(0,1).

The function hγ is a probability density function defined on (0, ∞) satisfying

0hγ(θ)dθ=1,0θvhγ(θ)dθ=Γ(1+v)Γ(1+γv),v[0,1].

We now list all the assumptions which will be applied in the whole paper.

(HA) The linear closed and densely defined operator A on X generates a compact C0 semigroup {T(t)}t > 0, and set M:=supt[0,c]T(t)<+.

(Hg) (1) g(t, y) is measurable in t on [0, c] for all yX, and continuous in y on X for a.e. t ∈ [0, c].

(2) For all yX and a.e. t ∈ [0, c], there exist a function ηLp([0, c], ℝ+) and a constant ρ with p > 1γ and 0<ρ<Γ(1+γ)cM such that

g(t,y)η(t)+ρt1γy.(2.1)

(HB) BL([0, c], 𝓛(Y, X)).

The set Uad for control functions is defined as

Uad={uLp([0,c],Y):u(t)U(t),a.e.t[0,c]},

where p > 1γ, and the multivalued map U : [0, c] → Pf(Y) (the set of all nonempty closed and convex subset of Y) satisfies the following condition (HU).

(HU) (1) U(⋅) is graph measurable.

(2) For a.e. t ∈ [0, c], there exists a function mLp([0, c], ℝ+) with p > 1γ such that

U(t)=sup{μ:μU(t)}m(t).

A noteworthy fact in [9] is that (HU) implies that Uad ≠ ∅, and obviously Uad is bounded, closed and convex. Moreover, ∥uLp ≤ ∥mLp and BuLp([0, c], X) for p > 1γ and uUad.

The following properties play an important role in this paper.

Lemma 2.1

Let 0 < γ < 1 and (HA) be satisfied. Then, the operator 𝓢γ(t) (t ≥ 0) defined in Definition 2.1 satisfies:

  1. {𝓢γ(t)}t ≥ 0 ⊆ 𝓛(X), and for each xX and t ≥ 0, there holds:

    Sγ(t)xγMΓ(1+γ)x.(2.2)
  2. for each xX, 𝓢γ(⋅)xC([0, c], X).

  3. for each t > 0, 𝓢γ(t) is a compact operator on X.

  4. the operator 𝓢γ(t) is continuous in the uniform operator topology for t > 0.

  5. limh0+1Γ(γ)Sγ(t+h)Sγ(t)Sγ(h)=0,t>0,limh0+1Γ(γ)Sγ(t)Sγ(h)Sγ(th)=0,t>0.

Proof

For the properties (1) (2) and (3), we refer to [33] for details. We now verify property (4). For 0 < t1 < t2, there exist positive numbers ϱ and N such that

Sγ(t2)Sγ(t1)γ0θhγ(θ)T(t2γθ)T(t1γθ)dθγ0ϱθhγ(θ)T(t2γθ)T(t1γθ)dθ+γϱNθhγ(θ)T(t2γθ)T(t1γθ)dθ+γNθhγ(θ)T(t2γθ)T(t1γθ)dθ2Mγ0ϱθhγ(θ)dθ+1Γ(γ)supθ[ϱ,N]T(t2γθ)T(t1γθ)+2MγNθhγ(θ)dθ.

The compactness of T(t) (t > 0) yields T(t2γθ)T(t1γθ)0 as t1t2 and θ ∈ [ϱ, N]. This together with the arbitrariness of ϱ and N as well as the fact 0θhγ(θ)dθ=1Γ(1+γ) gives that ∥𝓢γ(t2) − 𝓢γ(t1)∥ → 0 as t1t2.

For property (5), a similar manner as did in [6] gives the conclusion. This completes the proof. □

Lemma 2.2

If (HA) holds, then the operator F : Lp([0, c], X) → C1−γ([0, c], X) given by

(Fh)()=0(τ)γ1Sγ(τ)h(τ)dτ

is compact for p > 1γ.

Proof

For fixed r > 0, let BLp(r) = {hLp([0, c], X) : ∥hLpr}. We will show that the set {Fh : hBLp(r)} ⊆ C1−γ([0, c], X) is precompact, that is {⋅1−γFh(⋅) : hBLp(r)} ⊆ C([0, c], X) is precompact.

Firstly, we verify that {⋅1−γFh(⋅) : hBLp(r)} is equicontinuous. Let 0 ≤ t1} < t2} ≤ c and hBLp(r). If t1 = 0,

t21γFh(t2)t11γFh(t1)γMΓ(1+γ)t21γhLp([0,t2])(t2)γ1Lpp1([0,t2])γrMΓ(1+γ)(p1pγ1)11pt211p0,

as t2 → 0. If t1 > 0, for ϱ > 0 small enough with t1ϱ > 0, one has

t21γFh(t2)t11γFh(t1)t21γ0t1ϱ(t2τ)γ1Sγ(t2τ)Sγ(t1τ)h(τ)dτ+t21γt1ϱt1(t2τ)γ1Sγ(t2τ)Sγ(t1τ)h(τ)dτ+t21γt1t2(t2τ)γ1Sγ(t2τ)h(τ)dτ+t21γ0t1|(t2τ)γ1(t1τ)γ1|Sγ(t1τ)h(τ)dτ+[t21γt11γ]0t1(t1τ)γ1Sγ(t1τ)h(τ)dτc1γ(p1pγ1)11pr[t2pγ1p1(t2t1+ϱ)pγ1p1]11psupτ[0,t1ϱ]Sγ(t2τ)Sγ(t1τ)+c1γ2γMrΓ(1+γ)(p1pγ1)11p[(t2t1+ϱ)pγ1p1(t2t1)pγ1p1]11p+c1γγMrΓ(1+γ)(p1pγ1)11p(t2t1)γ1p+c1γγMrΓ(1+γ)(p1pγ1)11p[t1pγ1p1+(t2t1)pγ1p1t2pγ1p1]11p+[t21γt11γ]γMrΓ(1+γ)(p1pγ1)11pt1γ1p0,

as t2t1, due to the uniform continuity of 𝓢γ(t), t > 0 and the arbitrariness of ϱ.

Secondly, for each t ∈ [0, c], we prove that {t1−γFh(t) : hBLp(r)} is precompact in X. If t = 0, the conclusion is obvious. If t ∈ (0, c], for each ε > 0 with t − 2ε > 0, define the set {t1−γFεh(t) : hBLp(r)} in X, where

Fεh(t)=Γ(γ)Sγ(ε)0tε(tτ)γ1Sγ(tτε)h(τ)dτ.

Taking into account the compactness of 𝓢γ(ε), we obtain that the set {t1−γFεh(t) : hBLp(r)} is precompact in X. Moreover, for each hBLp(r), we have

t1γFh(t)t1γFεh(t)c1γ0t2ε(tτ)γ1[Sγ(tτ)Γ(γ)Sγ(ε)Sγ(tτε)]h(τ)dτ+c1γt2εt(tτ)γ1Sγ(tτ)h(τ)dτ+c1γΓ(γ)t2εtε(tτ)γ1Sγ(ε)Sγ(tτε)h(τ)dτc1γ(p1pγ1)11pr[tpγ1p1(2ε)pγ1p1]11psupτ[0,t2ε]Sγ(tτ)Γ(γ)Sγ(ε)Sγ(tτε)+c1γ(p1pγ1)11pγMrΓ(1+γ)(2ε)γ1p+c1γ(p1pγ1)11pM2rΓ(γ)[(2ε)pγ1p1εpγ1p1]11p0,

as ε → 0 by using the property (5) of Lemma 2.1. Then, the set {t1−γFh(t) : hBLp(r)} is precompact in X owning to the fact that the precompact set {t1−γFεh(t) : hBLp(r)} in X is close arbitrarily to it.

Finally, applying Ascoli-Arzela theorem, one gets that {⋅1−γFh(⋅) : hBLp(r)} is precompact in C([0, c], X), which means that {Fh(⋅) : hBLp(r)} is precompact in C1−γ([0, c], X). Then, we can come to the conclusion that F is compact. This completes the proof. □

3 The solvability of fractional differential system (1.1)

In this section, we derive the solvability of system (1.1) in the space C1−γ([0, c], X) by Schauder’s fixed point theorem.

Theorem 3.1

Let all the hypotheses listed in Section 2 be fulfilled. Then, for each uUad, system(1.1)possesses at least one mild solution in fC1−γ([0, c], X).

Proof

For each y0X and uUad, consider the operator 𝓠 : C1−γ([0, c], X) → C1−γ([0, c], X) as follows:

Qy(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,y(τ))+B(τ)u(τ)]dτ.

It is not difficult to verify that 𝓠 is well defined. Then, the solvability of system (1.1) will be transformed into a fixed point problem of 𝓠. For clarity, we proceed into the following steps.

Step 1. Let r > 0 and BC1−γ(r) = {yC1−γ([0, c], X) : ∥yC1−γr}. We show that 𝓠BC1−γ(r) ⊆ BC1−γ(r) provided that

r>Mγy0+Mγ[((p1)cpγ1)11p(ηLp+BuLp)]Γ(1+γ)Mρc.

In fact, for each yBC1−γ(r), one has

t1γQy(t)MγΓ(1+γ)y0+MγΓ(1+γ)[((p1)cpγ1)11p(ηLp+BuLp)+ρrcγ]r,

that is,

|QyC1γ=supt[0,c]t1γQy(t)r.

Step 2. We show that 𝓠 is continuous on BC1−γ(r). To this end, let {yn}n ≥1BC1−γ(r) with limnyn=yBC1γ(r), that is,

ynyC1γ=supt[0,c]t1γyn(t)y(t)0

as n → ∞. This yields t1−γyn(t) → t1−γy(t) as n → ∞ uniformly for t ∈ [0, c]. Note that, for a.e. τ ∈ [0, t],

g(τ,yn(τ))=g(τ,τγ1τ1γyn(τ))g(τ,τγ1τ1γy(τ))=g(τ,y(τ))

as n → ∞, and

g(τ,yn(τ))g(τ,y(τ))2(η(τ)+ρr),

where η(⋅) ∈ Lp}([0, c], ℝ+). Then, by applying the Lebesgue dominated convergence theorem, one has

t1γQyn(t)Qy(t)t1γ0t(tτ)γ1Sγ(tτ)[g(τ,yn(τ))g(τ,y(τ))]dτMγΓ(1+γ)((p1)cpγ1)11p(0cg(τ,yn(τ))g(τ,y(τ))pdτ)1p0,

as n → ∞ uniformly for each t ∈ [0, c], which means that

QynQyC1γ=supt[0,c]t1γQyn(t)Qy(t)0,n.

Step 3. We check the compactness of 𝓠 on C1−γ([0, c], X). The definition of 𝓠 yields that the compactness of 𝓠 is reduced to the compactness of 𝓠̃ on C1−γ([0, c], X), where

Q~y(t)=0t(tτ)γ1Sγ(tτ)g(τ,y(τ))dτ,t[0,c]

for each yC1−γ([0, c], X). It should be point out that (Hg)(2) implies that g(⋅, y(⋅)) ∈ Lp([0, c], X). A similar manner utilized in Lemma 2.2 gives the compactness of 𝓠̃.

Now, it is obvious that the conclusion of Theorem 3.1 holds by using the Schauder’s fixed point theorem. □

Remark 3.1

By virtue of Theorem 3.1, for each uUad, let yuC1−γ([0, c], X) be any one of the corresponding mild solutions of system (1.1). Then, ∥yu}∥C1−γR, where

R:=MγΓ(1+γ)[y0+((p1)cpγ1)11p(ηLp+BmLp)]Eγ(Mcρ),

which is independent of u, and Eγ(z)=n=0znΓ(nγ+1) is the Mittag-Leffler function. In fact, for each t ∈ [0, c], one has

t1γyu(t)Sγ(t)y0+t1γ0t(tτ)γ1Sγ(tτ)[g(τ,yu(τ))+B(τ)u(τ)]dτMγΓ(1+γ)[y0+((p1)cpγ1)11p(ηLp+BuLp)]+MγΓ(1+γ)c1γ0t(tτ)γ1ρτ1γyu(τ)dτ.

By using Corollary 2 of [31], one can obtain that

t1γyu(t)MγΓ(1+γ)[y0+((p1)cpγ1)11p(ηLp+BmLp)]Eγ(Mcρ).

This means that

yuC1γMγΓ(1+γ)[y0+((p1)cpγ1)11p(ηLp([0,c])+BmLp([0,c]))]Eγ(Mcρ).

Remark 3.2

For simplicity, we denote by

S(u)={yuBC1γ(R):yuismildsolutionof(1.1)correspondingtothecontroluUad},
Ad={(yu,u):uUad,yuS(u)}.

Remark 3.3

A pair (yu, u) is said to be feasible for the system (1.1) if and only if (yu, u) ∈ 𝓐d.

4 Time optimal control problems subjected to system (1.1)

Let WT be a bounded, closed and convex subset in X. Define the subsets as follows:

AdWT={(yu,u)Ad:t1γyu(t)WTfor somet[0,c]};U0={uUad:(yu,u)AdWTfor someyuS(u)};SuWT={yuS(u):uU0,(yu,u)AdWT}.

Suppose that AdWT ≠ ∅. For each (yu, u) ∈ AdWT, we define the transition time t(yu, u) as the first time such that t(yu,u)1γyu(t(yu,u))WT. The set WT is called the target set.

Remark 4.1

In general case, the subset AdWT is defined as:

A dWT={(yu,u)Ad:yu(t)WTfor somet[0,c]}.

However, since the solution is obtained in the space C1−γ([0, c], X) and yu(t) is indeed unbounded near the zero, a rescaling technique is necessary and a reasonable definition of AdWT in case of Riemann-Liouville derivatives is given as above.

Remark 4.2

For each (yu, u) ∈ AdWT, the definition of transition time gives

t(yu,u)=minT(yu,u),

where 𝓣(yu, u) := {t : t ∈ [0, c], t1−γyu(t) ∈ WT}. We claim that t(yu, u) is well defined. In fact, if the set 𝓣(yu, u) contains finite elements, the proof is trivial. Otherwise, let = inf 𝓣(yu, u). This gives that

limntn=t~

for some decreasing {tn}n ≥ 1 ⊆ 𝓣(yu, u), that is, tn1γyu(tn)WT. The fact ⋅1−γyu(⋅) ∈ C([0, c], X) yields

limntn1γyu(tn)=t~1γyu(t~).

This together with the closeness of WT gives

t~1γyu(t~)WT.

This means that = min 𝓣(yu, u), and t(yu, u) = .

Based on the above definitions and notations, now we consider the time optimal control problem (P): Find (y*, u*) ∈ AdWT such that

t(y,u)=min(yu,u)AdWTt(yu,u).

If the control u*, the time t(y*, u*) and the pair (y*, u*) exist solving problem (P), we call them time optimal control, optimal time and time optimal pair, respectively.

Theorem 4.1

Assume that all the hypotheses given in Section 2 are satisfied. Then, problem (P) possesses at least one time optimal pair.

Proof

In view of Theorem 3.1, there exists at least one yuBC1−γ(R) such that (yu, u) ∈ 𝓐d for each uUad. We will proceed in the following two steps to derive the main result.

Step 1. For each uU0, set tu=infyuSuWTt(yu,u). We now need to check that tu1γy^u(tu)WT for some y^uSuWT. It is trivial in situation in which the set SuWT has finite elements. Otherwise, there is a monotone decreasing sequence {t(ynu,u)}n1 such that

limnt(ynu,u)=tu,(4.1)

where (ynu,u)AdWT for each n ≥ 1. Moreover, the definition of t(ynu,u) gives

t(ynu,u)1γynu(t(ynu,u))WT.(4.2)

The fact ynuS(u) yields

ynu(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,ynu(τ))+B(τ)u(τ)]dτ(4.3)

for each n ≥ 1 and t ∈ (0, c]. Exploiting the compactness of 𝓢γ(t), t > 0, a similar method used in Lemma 2.2, we can infer that {ynu}n1 is precompact in C1−γ([0, c], X). Then, there is a subsequence of {ynu}n1, still relabled by it, and a function ŷuBC1−γ(R), such that

ynuy^uC1γ=supt[0,c]t1γynu(t)y^u(t)0(4.4)

as n → ∞. This together with (Hg) gives that

g(τ,ynu(τ))g(τ,y^u(τ)) and g(τ,ynu(τ))η(τ)+ρR

for a.e. τ ∈ [0, t], where η(⋅) ∈ Lp([0, c], ℝ+). Now, taking n → ∞ to both sides of (4.3) and using Lebesgue dominated convergence theorem yield

y^u(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,y^u(τ))+B(τ)u(τ)]dτ(4.5)

for each t ∈ (0, c]. This gives that

y^uS(u).(4.6)

It is worth noticing that (4.1) and (4.4) lead to

t(ynu,u)1γynu(t(ynu,u))tu1γy^u(tu)(4.7)

as n → ∞. In fact,

t(ynu,u)1γynu(t(ynu,u))tu1γy^u(tu)t(ynu,u)1γynu(t(ynu,u))t(ynu,u)1γy^u(t(ynu,u))+t(ynu,u)1γy^u(t(ynu,u))tu1γy^u(tu).

It follows from (4.4) that t(ynu,u)1γynu(t(ynu,u))t(ynu,u)1γy^u(t(ynu,u))0 as n → ∞. The fact ⋅1−γŷu(⋅) ∈ C([0, c], X) and (4.1) give t(ynu,u)1γy^u(t(ynu,u))tu1γy^u(tu)0 as n → ∞. (4.2) and (4.7), together with the closeness of WT give rise to the fact that

tu1γy^u(tu)WT.(4.8)

Combining this with (4.6) yields y^uSuWT.

Step 2. Put t=infuU0tu, where tu is the optimal time for fixed u in Step 1. Our task now is to seek an u*U0 and ySuWT such that t1γy(t)WT. The proof is trivial provided that U0 contains finite elements, or there exists a monotone decreasing sequence {tun}n ≥ 1 such that

limntun=t.(4.9)

According to Step 1, for each n ≥ 1, we can deduce that there is a function y^unSunWT such that

tun1γy^un(tun)WT,(4.10)

and

y^un(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,y^un(τ))+B(τ)un(τ)]dτ(4.11)

for each n ≥ 1 and t ∈ (0, c]. Note that B(⋅)un(⋅) ∈ Lp([0, c], X). So, an argument similar with the one employed in Lemma 2.2 gives rise to the precompactness of {ŷun}n ≥ 1 in C1−γ([0, c], X). Then, a subsequence of {ŷun}n ≥ 1 can be extracted, and still denoted by it, which satisfies

limny^un=y(4.12)

for some y*C1−γ([0, c], X). It is notable that {un}n ≥ 1UadLp([0, c], Y) and ∥unLp ≤ ∥mLp. The reflexivity of Y and the boundedness of {un}n ≥ 1 imply that a subsequence of {un}n ≥ 1, still relabled by it, satisfies

unu(4.13)

as n → ∞ for some u*Lp([0, c], Y). Owing to the fact that Uad is convex and closed, we can infer that u*Uad by using Mazur’s lemma. Thanks to Lemma 2.2, it is easy to deduce that

0t(tτ)γ1Sγ(tτ)B(τ)un(τ)dτ0t(tτ)γ1Sγ(tτ)B(τ)u(τ)dτ(4.14)

as n → ∞ since (4.13) holds. Now, making n → ∞ to both sides of (4.11) gives

y(t)=tγ1Sγ(t)y0+0t(tτ)γ1Sγ(tτ)[g(τ,y(τ))+B(τ)u(τ)]dτ(4.15)

for t ∈ (0, c], which implies that y*S(u*). We now turn back to (4.12). Together with (4.9), we have

tun1γy^un(tun)t1γy(t)(4.16)

as n → ∞, which means that t1γy(t)WT due to the closeness of WT and (4.10), and it is straight forward to see that ySuWT. This completes the proof. □

Remark 4.3

The new approach of constructing time minimizing sequences twice is applied to make up the lack of uniqueness of the mild solution. Thus, we can remove the Lipschitz continuity of nonlinear terms without any additional conditions. What is more, since the reflexivity of the state space X is no longer satisfied, we take full advantage of the compact method, and thus the time optimal pairs are still acquired. Therefore, the results here essentially generalize those in [10, 11, 14, 26, 29, 32], and the references therein, where the Lipschitz continuity of nonlinear function and the reflexivity of X are all required.

5 Applications

The following system concerned with the fractional Riemann-Liouville derivative will be considered here to illustrate our main results.

{34ω(t,θ)t34=2θ2ω(t,θ)+14t14sin(ω(t,θ))+0πζ(θ,τ)u(t,τ)dτ,t(0,1],θ[0,π],ω(t,0)=ω(t,π)=0,I14ω(t,θ)|t=0=ω0(θ).(5.1)

Let X = Y = L2([0, π], ℝ). Define the operator A : D(A) ⊆ XX as

Ax=x

with the domain

D(A)={xX;x,xare absolutely continuous,xX,x(0)=x(π)=0}.

Then,

Ax=n=1n2(x,ξn)ξn,xD(A),

where ξn(θ)=2πsin(nθ),n=1,2, is an orthonormal basis of X. By virtue of [25], we infer that A generates a compact and analytic semigroup {T(t)}t > 0 in X, and

T(t)x=n=1en2t(x,ξn)ξn,xX.

Obviously, ∥T(t)∥ ≤ 1.

Now, for every t ∈(0, 1], θ ∈ [0, π], let y(t)(θ) = ω(t, θ), g(t, y(t))(θ) = 14t14 sin(y(t)(θ)), uL2([0, 1] × [0, π], ℝ), u(t)(θ) = u(t, θ). ζC([0, π] × [0, π], ℝ), and B(t)u(t)(θ)=0πζ(θ,τ)u(t,τ)dτ.

Define admissible control set

U(t)={u(t)()Y:u(t)()YN1},

with N1 > 0. Then, fractional system (5.1) can be reformulated as the abstract fractional system (1.1), and we can prove that all the conditions listed in Section 2 are satisfied. In fact, c = 1 and M=supt[0,1]T(t)=1. Moreover,

g(t,y(t))()X=(0π14t14sin(y(t)(θ))2dθ)1214t14(0πy(t)(θ)2dθ)12=14t14y(t)()X,

with η(t) = 0 and ρ=14<Γ(74)Mc, and

B(t)u(t)()Xπsup0θπ|0πζ(θ,τ)u(t,τ)dτ|πsup0θπ|(0π|ζ(θ,τ)|2dτ)12(0π|u(t,τ)|2dτ)12au(t)()Y

for each t ∈ [0, 1], where a=πsup0θ,τπ|ζ(θ,τ)|. Define the target set

WT={xX:xXN2}

with N2 > 0. If the set AdWT ≠ ∅, then it follows from Theorem 4.1 that there exists a time optimal pair (y*, u*) such that the transition time t(y, u attains its minimum.

Acknowledgements

The work was supported by the NSF of China (11571300, 11771378), the Natural Science Foundation of the Jiangsu Higher education Institutions of China (18KJB110030) and the High-Level Personnel Support Program of Yangzhou University.

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Received: 2017-11-11
Published Online: 2019-02-09
Published in Print: 2018-12-19

© 2018 Diogenes Co., Sofia

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

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