Research Article Approximate Controllability of Fractional Sobolev-Type Evolution Equations in Banach Spaces

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Hindawi Publishing Corporation
Abstract and Applied Analysis
Volume 2013, Article ID 502839, 9 pages
http://dx.doi.org/10.1155/2013/502839
Research Article
Approximate Controllability of Fractional Sobolev-Type
Evolution Equations in Banach Spaces
N. I. Mahmudov
Eastern Mediterranean University, Gazimagusa, T.R. North Cyprus, Mersin 10, Turkey
Correspondence should be addressed to N. I. Mahmudov; nazim.mahmudov@emu.edu.tr
Received 3 January 2013; Accepted 1 February 2013
Academic Editor: Jen-Chih Yao
Copyright © 2013 N. I. Mahmudov. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We discuss the approximate controllability of semilinear fractional Sobolev-type differential system under the assumption that the
corresponding linear system is approximately controllable. Using Schauder fixed point theorem, fractional calculus and methods
of controllability theory, a new set of sufficient conditions for approximate controllability of fractional Sobolev-type differential
equations, are formulated and proved. We show that our result has no analogue for the concept of complete controllability. The
results of the paper are generalization and continuation of the recent results on this issue.
1. Introduction
Many social, physical, biological, and engineering problems
can be described by fractional partial differential equations.
In fact, fractional differential equations are considered as an
alternative model to nonlinear differential equations. In the
last two decades, fractional differential equations (see Samko
et al. [1] and the references therein) have attracted many
scientists, and notable contributions have been made to both
theory and applications of fractional differential equations.
Recently, the existence of mild solutions and stability
and (approximate) controllability of (fractional) semilinear
evolution system in Banach spaces have been reported by
many researchers; see [2–36]. We refer the reader to ElBorai [3, 4], Balachandran and Park [5], Zhou and Jiao [6, 7]
Hernández et al. [8], Wang and Zhou [9], Sakthivel et al. [12,
13], Debbouche and Baleanu [14], Wang et al. [15–21], Kumar
and Sukavanam [22], Li and Yong [37], Dauer and Mahmudov [28], Mahmudov [27, 29], and the references therein.
Complete controllability of evolution systems of Sobolev type
in Banach spaces has been studied by Balachandran and
Dauer [23], Ahmed [24], and Feckan et al. [2]. However, the
approximate controllability of fractional evolution equations
of Sobolev type has not been studied.
Motivated by the above-mentioned papers, we study the
approximate controllability of a class of fractional evolution
equations of Sobolev type:
𝑐
𝐷𝑑𝛼 (𝐸π‘₯ (𝑑)) = 𝐴π‘₯ (𝑑) + 𝐡𝑒 (𝑑) + 𝑓 (𝑑, π‘₯ (𝑑)) ,
𝑑 ∈ [0, 𝑏] ,
π‘₯ (0) = π‘₯0 ,
(1)
where 𝐴 : 𝐷 (𝐴) ⊂ 𝑋 → 𝑋 and 𝐸 : 𝐷 (𝐸) ⊂ 𝑋 →
𝑋 are linear operators from a Banach space 𝑋 to 𝑋. The
control function 𝑒 takes values in a Hilbert space π‘ˆ and 𝑒 ∈
𝐿2 ([0, 𝑏], π‘ˆ). 𝐡 : π‘ˆ → 𝑋 is a linear bounded operator. The
function 𝑓 ∈ 𝐢 ([0, 𝑏] × π‘‹, 𝑋) will be specified in the sequel.
The fractional derivative 𝑐 𝐷𝑑𝛼 , 0 < 𝛼 < 1, is understood in
the Caputo sense.
Our aim in this paper is to provide a sufficient condition
for the approximate controllability for a class of fractional
evolution equations of Sobolev type. It is assumed that
𝐸−1 is compact, and, consequently, the associated linear
control system (35) is not exactly controllable. Therefore, our
approximate controllability results have no analogue for the
concept of complete controllability. In Section 5, we give an
2
Abstract and Applied Analysis
example of the system which is not completely controllable,
but approximately controllable.
For π‘₯ ∈ 𝑋 and 0 < 𝛼 < 1, we define two families {S𝐸 (𝑑) :
𝑑 ≥ 0} and {T𝐸 (𝑑) : 𝑑 ≥ 0} of operators by
∞
S𝛼 (𝑑) = ∫ Ψ𝛼 (πœƒ) 𝑆 (𝑑𝛼 πœƒ) π‘‘πœƒ, T𝛼 (𝑑)
2. Preliminaries
0
Throughout this paper, unless otherwise specified, the following notations will be used. Let 𝑋 be a separable reflexive
Banach space and let 𝑋∗ stand for its dual space with respect
to the continuous pairing ⟨⋅, ⋅⟩. We may assume, without loss
of generality, that 𝑋 and 𝑋∗ are smooth and strictly convex,
by virtue of a renorming theorem (see, e.g., [37, 38]). In
particular, this implies that the duality mapping 𝐽 of 𝑋 into
𝑋∗ given by the relations
‖𝐽 (𝑧)β€–∗ = ‖𝑧‖ ,
⟨𝐽 (𝑧) , π‘§βŸ© = ‖𝑧‖2 ,
∀𝑧 ∈ 𝑋
(S1) 𝐴 and 𝐸 are linear operators, and 𝐴 is closed;
(S2) 𝐷(𝐸) ⊂ 𝐷(𝐴) and 𝐸 is bijective;
(S3) 𝐸−1 : 𝑋 → 𝐷(𝐸) is compact.
The hypotheses (S1)–(S3) and the closed graph theorem
imply the boundedness of the linear operator 𝐴𝐸−1 : 𝑋 →
𝑋. Consequently, −𝐴𝐸−1 generates a semigroup {𝑆(𝑑); 𝑑 ≥ 0}
in 𝑋. Assume that max0≤𝑑≤𝑏 ‖𝑆(𝑑)β€– =: 𝑀.
Let us recall the following known definitions in fractional
calculus. For more details, see [1].
Definition 1. The fractional integral of order 𝛼 > 0 with the
lower limit 0 for a function 𝑓 is defined as
𝑑
𝑓(𝑠)
1
𝑑𝑠,
∫
Γ (𝛼) 0 (𝑑 − 𝑠)1−𝛼
𝑑 > 0, 𝛼 > 0,
(3)
Definition 2. The Caputo derivative of order 𝛼 for a function
𝑓 can be written as
𝐷𝛼 𝑓 (𝑑) =
(𝑛)
𝑑
𝑓 (𝑠)
1
𝑑𝑠
∫
Γ (𝑛 − 𝛼) 0 (𝑑 − 𝑠)1+𝛼−𝑛
=𝐼
𝑛−𝛼 (𝑛)
𝑓
(𝑑) ,
S𝐸 (𝑑) = 𝐸−1 S𝛼 (𝑑) ,
T𝐸 (𝑑) = 𝐸−1 T𝛼 (𝑑) ,
where
Ψ𝛼 (πœƒ) =
1 ∞
Γ (𝑛𝛼 + 1)
sin (π‘›πœ‹π›Ό) ,
∑ (−1)𝑛−1
πœ‹π›Ό 𝑛=1
𝑛!
πœƒ ∈ (0, ∞) ,
is the function of Wright type defined on (0, ∞), which
satisfies
Ψ𝛼 (πœƒ) ≥ 0,
∞
∞
∫ Ψ𝛼 (πœƒ) π‘‘πœƒ = 1,
0
à (1 + 𝜁)
,
∫ πœƒ Ψ𝛼 (πœƒ) π‘‘πœƒ =
Γ (1 + π›Όπœ)
0
𝜁
(7)
𝜁 ∈ (−1, ∞) .
Lemma 3 (see [2]). The operators S𝐸 and T𝐸 have the following properties.
(i) For any fixed 𝑑 ≥ 0, 𝑆𝐸 (𝑑) and 𝑇𝐸 (𝑑) are linear and
bounded operators, and
σ΅„© −1 σ΅„©
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©S𝐸 (𝑑) π‘₯σ΅„©σ΅„©σ΅„© ≤ 𝑀 󡄩󡄩󡄩󡄩𝐸 σ΅„©σ΅„©σ΅„©σ΅„© β€–π‘₯β€– ,
σ΅„©σ΅„© −1 σ΅„©σ΅„©
(8)
σ΅„©σ΅„©
σ΅„©σ΅„© 𝑀 󡄩󡄩󡄩𝐸 σ΅„©σ΅„©σ΅„©
β€–π‘₯β€– .
σ΅„©σ΅„©T𝐸 (𝑑) π‘₯σ΅„©σ΅„© ≤
Γ (𝛼)
(ii) {S𝐸 (𝑑) : 𝑑 ≥ 0} and {T𝐸 (𝑑) : 𝑑 ≥ 0} are compact.
In this paper, we adopt the following definition of mild
solution of (1).
Definition 4. A solution π‘₯(⋅; 𝑒) ∈ 𝐢([0, 𝑏], 𝑋) is said to be a
mild solution of (1) if for any 𝑒 ∈ 𝐿2 ([0, 𝑏], π‘ˆ), the integral
equation
π‘₯ (𝑑) = S𝐸 (𝑑) 𝐸π‘₯0
provided the right-hand side is pointwise defined on [0, ∞),
where Γ is the gamma function.
𝑐
(5)
0
(6)
(2)
is bijective, homogeneous, demicontinuous, that is, continuous from 𝑋 with a strong topology, into 𝑋∗ with weak
topology, and strictly monotonic. Moreover, 𝐽−1 : 𝑋∗ → 𝑋
is also duality mapping.
The operators 𝐴 : 𝐷 (𝐴) ⊂ 𝑋 → 𝑋 and 𝐸 : 𝐷 (𝐸) ⊂
𝑋 → 𝑋 satisfy the following hypotheses:
𝐼𝛼 𝑓 (𝑑) =
∞
= 𝛼 ∫ πœƒΨ𝛼 (πœƒ) 𝑆 (𝑑𝛼 πœƒ) π‘‘πœƒ,
(4)
𝑑 > 0, 𝑛 − 1 ≤ 𝛼 < 𝑛.
If 𝑓 is an abstract function with values in 𝑋, then integrals
which appear in the above definitions are taken in Bochner’s
sense.
𝑑
+ ∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) [𝐡𝑒 (𝑠) + 𝑓 (𝑠, π‘₯ (𝑠))] 𝑑𝑠
(9)
0
is satisfied.
Let π‘₯(𝑏; 𝑒) be the state value of (9) at terminal time 𝑏
corresponding to the control 𝑒. Introduce the set R(𝑏) =
{π‘₯(𝑏; 𝑒) : 𝑒 ∈ 𝐿 2 ([0, 𝑏], π‘ˆ)}, which is called the reachable set
of system (9) at terminal time 𝑏; its closure in 𝑋 is denoted by
R(𝑏).
Definition 5. System (1) is said to be approximately controllable on [0, 𝑏] if R(𝑏) = 𝑋; that is, given an arbitrary πœ€ > 0,
it is possible to steer from the point π‘₯0 to within a distance πœ€
from all points in the state space 𝑋 at time 𝑏.
Abstract and Applied Analysis
3
To investigate the approximate controllability of system
(9), we assume the following conditions.
(H4) The function 𝑓 : [0, 𝑏]×𝑋 → 𝑋 satisfies the following:
(a) 𝑓(𝑑, ⋅) : 𝑋 → 𝑋 is continuous for each 𝑑 ∈ [0, 𝑏]
and for each π‘₯ ∈ 𝑋, 𝑓(⋅, π‘₯) : [0, 𝑏] → 𝑋 is
strongly measurable;
(b) there is a positive integrable function 𝑛 ∈
𝐿1 ([0, 𝑏], [0, +∞)) and a continuous nondecreasing function Λ π‘“ : [0, ∞) → (0, ∞) such
that for every (𝑑, π‘₯) ∈ [0, 𝑏] × π‘‹, we have
󡄩󡄩󡄩𝑓 (𝑑, π‘₯)σ΅„©σ΅„©σ΅„© ≤ 𝑛 (𝑑) Λ π‘“ (β€–π‘₯β€–) ,
σ΅„©
σ΅„©
(10)
Λ π‘“ (π‘Ÿ)
lim inf
= πœŽπ‘“ < ∞.
π‘Ÿ→∞
π‘Ÿ
(H5) The following relationship holds:
σ΅„©σ΅„© −1 σ΅„©σ΅„©
1 2 2 𝑏2𝛼−1 𝑀 󡄩󡄩󡄩𝐸 σ΅„©σ΅„©σ΅„© 𝑏𝛼
(1 + 𝑀𝐡 𝑀T
)
πœ€
2𝛼 − 1
Γ (𝛼) 𝛼
Having noticed this fact, our goal, in this section, is to find
conditions for the solvability of (14). It will be shown that the
control in (14) drives system (1) from π‘₯0 to
−1
β„Ž − πœ€π½ ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯)) ,
provided that system (14) has a solution.
Theorem 6. Assume that assumptions (S1)–(S3), (H4), (H5)
hold and 1/2 < 𝛼 ≤ 1. Then there exists a solution to (14).
Proof. The proof of Theorem 6 follows from Lemmas 7–9,
infinite dimensional analogue of Arzela-Ascoli theorem, and
the Schauder fixed point theorem.
For all πœ€ > 0, consider the operator Φπœ€ : 𝐢 ([0, 𝑏], 𝑋) →
𝐢 ([0, 𝑏], 𝑋) defined as follows:
(11)
(Φπœ€ π‘₯) (𝑑)
× πœŽπ‘“ sup 𝑛 (𝑠) < 1,
𝑑
:= S𝐸 (𝑑) 𝐸π‘₯0 + ∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠)
𝑠∈[0,𝑏]
here 𝑀𝐡 := ‖𝐡‖, 𝑀T := β€–T𝐸 β€–.
0
× [π΅π‘’πœ€ (𝑠, π‘₯) + 𝑓 (𝑠, π‘₯ (𝑠))] 𝑑𝑠,
(17)
−1
(H6) For every β„Ž ∈ 𝑋, 𝑧𝛼 (β„Ž) = πœ€(πœ€πΌ + Γ0𝑏 𝐽) (β„Ž) converges
to zero as πœ€ → 0+ in strong topology, where
𝑏
Γ0𝑏 := ∫ (𝑏 − 𝑠)2(𝛼−1) T𝐸 (𝑏 − 𝑠) 𝐡𝐡∗ T∗𝐸 (𝑏 − 𝑠) 𝑑𝑠,
0
(12)
and π‘§πœ€ (β„Ž) is a solution of
(13)
−1
π‘’πœ€ (𝑑, π‘₯) = (𝑏 − 𝑑)𝛼−1 𝐡∗ T∗𝐸 (𝑏 − 𝑑) 𝐽 ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯)) ,
𝑏
− ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝑓 (𝑠, π‘₯ (𝑠)) 𝑑𝑠.
0
3. Existence Theorem
In order to formulate the controllability problem in the
form suitable for application of fixed point theorem, it is
assumed that the corresponding linear system is approximately controllable. Then it will be shown that system (1)
is approximately controllable if for all πœ€ > 0, there exists a
continuous function π‘₯ ∈ 𝐢 ([0, 𝑏], 𝑋) such that
−1
π‘’πœ€ (𝑑, π‘₯) = (𝑏 − 𝑑)𝛼−1 𝐡∗ T∗𝐸 (𝑏 − 𝑑) 𝐽 ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯)) ,
0 ≤ 𝑑 < 𝑏,
π‘₯ (𝑑) = S𝐸 (𝑑) 𝐸π‘₯0
𝑑
+ ∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) [𝐡𝑒 (𝑠) + 𝑓 (𝑠, π‘₯ (𝑠))] 𝑑𝑠,
0
(14)
where
𝑝 (π‘₯) = β„Ž − S𝐸 (𝑏) 𝐸π‘₯0
− ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝑓 (𝑠, π‘₯ (𝑠)) 𝑑𝑠.
0
where
𝑝 (π‘₯) = β„Ž − S𝐸 (𝑏) 𝐸π‘₯0
πœ€π‘§πœ€ + Γ0𝑏 𝐽 (π‘§πœ€ ) = πœ€β„Ž.
𝑏
(16)
(15)
(18)
It will be shown that for all πœ€ > 0, the operator Φπœ€ :
𝐢 ([0, 𝑏], 𝑋) → 𝐢 ([0, 𝑏], 𝑋) has a fixed point. To prove this
we will employ the Schauder fixed point theorem.
Lemma 7. Under assumptions (S1)–(S3), (H4), (H5), for any
πœ€ > 0 there exists a positive number π‘Ÿ := π‘Ÿ(πœ€) such that
Φπœ€ (π΅π‘Ÿ ) ⊂ π΅π‘Ÿ .
Proof. Let πœ€ > 0 be fixed. If it is not true, then for each π‘Ÿ > 0,
there exists a function π‘§π‘Ÿ ∈ π΅π‘Ÿ , but Φπœ€ (π‘§π‘Ÿ ) ∉ π΅π‘Ÿ . So for some
𝑑 = 𝑑(π‘Ÿ) ∈ [0, 𝑏], one can show that
σ΅„©
σ΅„©
σ΅„© σ΅„©
π‘Ÿ ≤ σ΅„©σ΅„©σ΅„©(Φπœ€ π‘§π‘Ÿ ) (𝑑)σ΅„©σ΅„©σ΅„© ≤ σ΅„©σ΅„©σ΅„©S𝐸 (𝑑) 𝐸π‘₯0 σ΅„©σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©σ΅„© 𝑑
σ΅„©
+ σ΅„©σ΅„©σ΅„©∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯ (𝑠)) 𝑑𝑠󡄩󡄩󡄩
σ΅„©σ΅„© 0
σ΅„©σ΅„©
σ΅„©σ΅„©σ΅„© 𝑑
σ΅„©σ΅„©σ΅„©
+ σ΅„©σ΅„©σ΅„©∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) π΅π‘’πœ€ (𝑠, π‘₯) 𝑑𝑠󡄩󡄩󡄩
σ΅„©σ΅„© 0
σ΅„©σ΅„©
= : 𝐼1 + 𝐼2 + 𝐼3 .
(19)
4
Abstract and Applied Analysis
Let us estimate 𝐼𝑖 , 𝑖 = 1, 2, 3. By the assumption (H4), we
have
σ΅„© σ΅„©σ΅„©
σ΅„©
σ΅„©
σ΅„©
𝐼1 ≤ σ΅„©σ΅„©σ΅„©S𝐸 (𝑑) 𝐸π‘₯0 σ΅„©σ΅„©σ΅„© ≤ 𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„© 󡄩󡄩󡄩𝐸π‘₯0 σ΅„©σ΅„©σ΅„© ,
(20)
𝑑
σ΅„©
σ΅„©
𝐼2 ≤ ∫ σ΅„©σ΅„©σ΅„©σ΅„©(𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯ (𝑠))σ΅„©σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
≤
σ΅„© σ΅„©
𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„©
𝑑
σ΅„© σ΅„©
2𝛼−1
𝑀 󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„© 𝑏𝛼
1
2 𝑏
) σ΅„© σ΅„© πœŽπ‘“ sup 𝑛 (𝑠) ≥ 1, (25)
(1 + 𝑀𝐡2 𝑀T
πœ€
2𝛼 − 1
Γ (𝛼) 𝛼 𝑠∈[0,𝑏]
which is a contradiction by assumption (H5). Thus, Φπœ€ (π΅π‘Ÿ ) ⊂
π΅π‘Ÿ for some π‘Ÿ > 0.
σ΅„©
σ΅„©
∫ (𝑑 − 𝑠)𝛼−1 󡄩󡄩󡄩𝑓 (𝑠, π‘₯ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠
Γ (𝛼)
0
σ΅„©σ΅„© −1 σ΅„©σ΅„© 𝑑
𝑀 󡄩󡄩󡄩𝐸 σ΅„©σ΅„©σ΅„©
≤
∫ (𝑑 − 𝑠)𝛼−1 𝑛 (𝑠) Λ π‘“ (β€–π‘₯ (𝑠)β€–) 𝑑𝑠
Γ (𝛼)
0
σ΅„©σ΅„© −1 σ΅„©σ΅„© 𝛼
𝑀 󡄩󡄩󡄩𝐸 σ΅„©σ΅„©σ΅„© 𝑏
≤
Λ (π‘Ÿ) sup 𝑛 (𝑠) .
Γ (𝛼) 𝛼 𝑓
𝑠∈𝐽
Dividing both sides by π‘Ÿ and taking π‘Ÿ → ∞, we obtain that
(21)
Lemma 8. Let assumptions (S1)–(S3), (H4), (H5) hold. Then
the set {Φπœ€ 𝑧 : 𝑧 ∈ π΅π‘Ÿ } is an equicontinuous family of functions
on [0, 𝑏].
Proof. Let 0 < πœ‚ < 𝑑 < 𝑏 and 𝛿 > 0 such that
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©T𝐸 (𝑠1 ) − T𝐸 (𝑠2 )σ΅„©σ΅„©σ΅„© < πœ‚
Combining the estimates (19)–(21) yields
σ΅„© σ΅„©σ΅„©
σ΅„©
𝐼1 + 𝐼2 < 𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„© 󡄩󡄩󡄩𝐸π‘₯0 σ΅„©σ΅„©σ΅„©
σ΅„© σ΅„©
𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„© 𝑏𝛼
+
Λ (π‘Ÿ) sup 𝑛 (𝑠) := Δ.
Γ (𝛼) 𝛼 𝑓 𝑠∈[0,𝑏]
(22)
𝑑
σ΅„©
σ΅„©
𝐼3 ≤ ∫ σ΅„©σ΅„©σ΅„©σ΅„©(𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) π΅π‘’πœ€ (𝑠, π‘₯)σ΅„©σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
σ΅„©σ΅„©
= ∫ σ΅„©σ΅„©σ΅„©(𝑑 − 𝑠)𝛼−1 (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠)
0 σ΅„©
𝑑
σ΅„©σ΅„©
σ΅„©
× T𝐸 (𝑑 + β„Ž − 𝑠) [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] 𝑑𝑠󡄩󡄩󡄩
σ΅„©σ΅„©
σ΅„©σ΅„©
−1
×𝐡𝐡∗ T∗𝐸 (𝑏 − 𝑑) 𝐽 ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯))σ΅„©σ΅„©σ΅„© 𝑑𝑠
σ΅„©
𝑑
σ΅„©
σ΅„©
≤ ∫ σ΅„©σ΅„©σ΅„©σ΅„©(𝑑 − 𝑠)𝛼−1 (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠) 𝐡𝐡∗ T∗𝐸 (𝑏 − 𝑑)σ΅„©σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
σ΅„©σ΅„©
σ΅„©σ΅„©
−1
× σ΅„©σ΅„©σ΅„©π½ ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯))σ΅„©σ΅„©σ΅„©
σ΅„©
σ΅„©
σ΅„©σ΅„©
𝑏2𝛼−1 σ΅„©σ΅„©σ΅„©
𝑏 −1
󡄩󡄩𝐽 ((πœ€πΌ + Γ0 𝐽) 𝑝 (π‘₯))σ΅„©σ΅„©σ΅„©
σ΅„©
σ΅„©
2𝛼 − 1
2
= 𝑀𝐡2 𝑀T
σ΅„©σ΅„©
𝑏2𝛼−1 σ΅„©σ΅„©σ΅„©
𝑏 −1
σ΅„©(πœ€πΌ + Γ0 𝐽) 𝑝 (π‘₯)σ΅„©σ΅„©σ΅„©
σ΅„©
2𝛼 − 1 σ΅„©σ΅„©
≤
1 2 2 𝑏2𝛼−1 σ΅„©σ΅„©
σ΅„©
𝑀 𝑀
󡄩𝑝 (π‘₯)σ΅„©σ΅„©σ΅„©
πœ€ 𝐡 T 2𝛼 − 1 σ΅„©
≤
1 2 2 𝑏2𝛼−1
𝑀 𝑀
Δ.
πœ€ 𝐡 T 2𝛼 − 1
for every 𝑠1 , 𝑠2 ∈ [0, 𝑏] with |𝑠1 − 𝑠2 | < 𝛿. For 𝑧 ∈ π΅π‘Ÿ , 0 < |β„Ž| <
𝛿, 𝑑 + β„Ž ∈ [0, 𝑏], we have
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©(Φπœ€ 𝑧) (𝑑 + β„Ž) − (Φπœ€ 𝑧) (𝑑)σ΅„©σ΅„©σ΅„©
σ΅„©σ΅„© 𝑑
σ΅„©
≤ σ΅„©σ΅„©σ΅„©∫ ((𝑑 + β„Ž − 𝑠)𝛼−1 − (𝑑 − 𝑠)𝛼−1 )
σ΅„©σ΅„© 0
On the other hand,
2
≤ 𝑀𝐡2 𝑀T
σ΅„©σ΅„© 𝑑+β„Ž
σ΅„©
+ σ΅„©σ΅„©σ΅„©σ΅„©∫ (𝑑 + β„Ž − 𝑠)𝛼−1 T𝐸 (𝑑 + β„Ž − 𝑠)
σ΅„©σ΅„© 𝑑
σ΅„©σ΅„©
σ΅„©
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] 𝑑𝑠󡄩󡄩󡄩󡄩
σ΅„©σ΅„©
σ΅„©σ΅„© 𝑑
σ΅„©
+ σ΅„©σ΅„©σ΅„©∫ (𝑑 − 𝑠)𝛼−1 (T𝐸 (𝑑 + β„Ž − 𝑠) − T𝐸 (𝑑 − 𝑠))
σ΅„©σ΅„© 0
σ΅„©σ΅„©
σ΅„©
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] 𝑑𝑠󡄩󡄩󡄩 .
σ΅„©σ΅„©
Applying Lemma 3 and the Holder inequality, we obtain
(23)
Thus,
2𝛼−1
1
σ΅„©
σ΅„©
2 𝑏
Δ
π‘Ÿ ≤ σ΅„©σ΅„©σ΅„©(Φπœ€ π‘§π‘Ÿ ) (𝑑)σ΅„©σ΅„©σ΅„© ≤ Δ + 𝑀𝐡2 𝑀T
πœ€
2𝛼 − 1
2𝛼−1
1
2 𝑏
= (1 + 𝑀𝐡2 𝑀T
) Δ.
πœ€
2𝛼 − 1
(26)
σ΅„©σ΅„©
σ΅„©
σ΅„©σ΅„©(Φπœ€ 𝑧) (𝑑 + β„Ž) − (Φπœ€ 𝑧) (𝑑)σ΅„©σ΅„©σ΅„©
σ΅„© σ΅„©
𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„©
≤
Λ π‘“ (π‘Ÿ)
Γ (𝛼)
𝑑
× ∫ ((𝑑 + β„Ž − 𝑠)𝛼−1 − (𝑑 − 𝑠)𝛼−1 ) 𝑛 (𝑠) 𝑑𝑠
0
(24)
+
σ΅„© σ΅„©
𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„© 1
Γ (𝛼)
πœ€
𝑀𝐡 𝑀T Δ
(27)
Abstract and Applied Analysis
5
σ΅„©σ΅„© 𝑑
∞
σ΅„©
+ 𝛼 σ΅„©σ΅„©σ΅„©∫ ∫ πœƒ(𝑑 − 𝑠)𝛼−1 Ψ𝛼 (πœƒ) 𝑆 ((𝑑 − 𝑠)𝛼 πœƒ)
σ΅„©σ΅„© 𝑑−πœ† 𝛿
𝑑
× ∫ ((𝑑 + β„Ž − 𝑠)𝛼−1 − (𝑑 − 𝑠)𝛼−1 ) (𝑏 − 𝑠)𝛼−1 𝑑𝑠
0
σ΅„© σ΅„©
𝑀 󡄩󡄩󡄩󡄩𝐸−1 σ΅„©σ΅„©σ΅„©σ΅„©
𝑑+β„Ž
Λ π‘“ (π‘Ÿ) ∫ (𝑑 + β„Ž − 𝑠)
Γ (𝛼)
𝑑
σ΅„©σ΅„© −1 σ΅„©σ΅„©
𝑀 󡄩󡄩𝐸 σ΅„©σ΅„© 1
+ σ΅„© σ΅„© 𝑀𝐡 𝑀T Δ
Γ (𝛼) πœ€
+
×∫
𝑑+β„Ž
𝑑
𝛼−1
σ΅„©σ΅„©
σ΅„©
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] π‘‘πœƒ 𝑑𝑠󡄩󡄩󡄩
σ΅„©σ΅„©
𝑛 (𝑠) 𝑑𝑠
= : 𝐽1 + 𝐽2 .
(30)
A similar argument, as before, is as follows:
(𝑑 + β„Ž − 𝑠)𝛼−1 (𝑏 − 𝑠)𝛼−1 𝑑𝑠
𝑑
πœ‚π‘‡π›Ό
πœ‚π‘‡π›Ό 1
+
Λ π‘“ (π‘Ÿ) ∫ (𝑑 − 𝑠)𝛼−1 𝑛 (𝑠) 𝑑𝑠 +
𝑀 𝑀 Δ
𝛼
𝛼 πœ€ 𝐡 T
0
𝑑
× ∫ (𝑑 − 𝑠)
0
𝛼−1
(𝑏 − 𝑠)
𝛼−1
𝑑
σ΅„©
σ΅„© σ΅„©
σ΅„©
𝐽1 ≤ 𝛼𝑀 ∫ (𝑑 − 𝑠)𝛼−1 (σ΅„©σ΅„©σ΅„©π΅π‘’πœ€ (𝑠, 𝑧)σ΅„©σ΅„©σ΅„© + 󡄩󡄩󡄩𝑓 (𝑠, 𝑧 (𝑠))σ΅„©σ΅„©σ΅„©) 𝑑𝑠
0
𝛿
× (∫ πœƒΨ𝛼 (πœƒ) π‘‘πœƒ)
𝑑𝑠.
0
(28)
𝑑
1
≤ 𝛼𝑀 ( 𝑀𝐡 𝑀T Δ ∫ (𝑑 − 𝑠)𝛼−1 (𝑏 − 𝑠)𝛼−1 𝑑𝑠
πœ€
0
Therefore, for πœ€ sufficiently small, the right-hand side of
(28) tends to zero as β„Ž → 0. On the other hand, the
compactness of T𝐸 (𝑑), 𝑑 > 0, implies the continuity in the
uniform operator topology. Thus, the set {Φπœ€ 𝑧 : 𝑧 ∈ π΅π‘Ÿ } is
equicontinuous.
Lemma 9. Let assumptions (S1)–(S3), (H4), (H5) hold. Then
Φπœ€ maps π΅π‘Ÿ onto a precompact set in π΅π‘Ÿ .
Proof. Let 0 < 𝑑 ≤ 𝑏 be fixed and let πœ† be a real number
satisfying 0 < πœ† < 𝑑. For 𝛿 > 0, define an operator Φπœ†,𝛿
πœ€ on π΅π‘Ÿ
by
= 𝛼∫
0
0
0
𝑑
𝐽2 ≤ 𝛼𝑀 ∫
𝑑−πœ†
σ΅„©
σ΅„© σ΅„©
σ΅„©
(𝑑 − 𝑠)𝛼−1 (σ΅„©σ΅„©σ΅„©π΅π‘’πœ€ (𝑠, 𝑧)σ΅„©σ΅„©σ΅„© + 󡄩󡄩󡄩𝑓 (𝑠, 𝑧 (𝑠))σ΅„©σ΅„©σ΅„©) 𝑑𝑠
∞
× (∫ πœƒπœ‚π›Ό (πœƒ) π‘‘πœƒ)
𝛿
≤
𝑑
1
𝛼𝑀
( 𝑀𝐡 𝑀T Δ ∫ (𝑑 − 𝑠)𝛼−1 (𝑏 − 𝑠)𝛼−1 𝑑𝑠
Γ (1 + 𝛼) πœ€
𝑑−πœ†
𝑑
𝑑−πœ†
(32)
(𝑑 − 𝑠)𝛼−1 𝑛 (𝑠) 𝑑𝑠) ,
∞
𝐸−1 ∫ πœƒ(𝑑 − 𝑠)𝛼−1 Ψ𝛼 (πœƒ) 𝑆 ((𝑑 − 𝑠)𝛼 πœƒ)
where we have used the equality
𝛿
= 𝛼𝐸−1 𝑆 (πœ†π›Ό 𝛿)
𝑑−πœ†
0
+Λ π‘“ (π‘Ÿ) ∫
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] 𝑑𝑠
×∫
𝛿
(31)
(Φπœ†,𝛿
πœ€ 𝑧) (𝑑)
𝑑−πœ†
𝑑
+Λ π‘“ (π‘Ÿ) ∫ (𝑑 − 𝑠)𝛼−1 𝑛 (𝑠) 𝑑𝑠) (∫ πœƒΨ𝛼 (πœƒ) π‘‘πœƒ) ,
∞
(29)
∞
∫ πœƒ(𝑑 − 𝑠)𝛼−1 Ψ𝛼 (πœƒ) 𝑆 ((𝑑 − 𝑠)𝛼 πœƒ − πœ†π›Ό 𝛿)
𝛿
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] 𝑑𝑠.
Since 𝐸−1 is a compact operator, the set {(Φπœ†,𝛿
πœ€ 𝑧)(𝑑) : 𝑧 ∈ π΅π‘Ÿ }
is precompact in 𝑋 for every 0 < πœ† < 𝑑, 𝛿 > 0. Moreover, for
each 𝑧 ∈ π΅π‘Ÿ , we have
σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©(Φπœ€ 𝑧) (𝑑) − (Φπœ†,𝛿
σ΅„©
πœ€ 𝑧) (𝑑)σ΅„©
σ΅„©
σ΅„©
σ΅„©σ΅„© 𝑑 𝛿
σ΅„©
≤ 𝛼 σ΅„©σ΅„©σ΅„©σ΅„©∫ ∫ πœƒ(𝑑 − 𝑠)𝛼−1 Ψ𝛼 (πœƒ) 𝑆 ((𝑑 − 𝑠)𝛼 πœƒ)
σ΅„©σ΅„© 0 0
σ΅„©σ΅„©
σ΅„©
× [π΅π‘’πœ€ (𝑠, 𝑧) + 𝑓 (𝑠, 𝑧 (𝑠))] π‘‘πœƒ 𝑑𝑠󡄩󡄩󡄩󡄩
σ΅„©σ΅„©
∫ πœƒπ›Όπ›½ Ψ𝛼 (πœƒ) π‘‘πœƒ =
0
Γ (1 + 𝛽)
.
Γ (1 + 𝛼𝛽)
(33)
From (30)–(32), one can see that for each 𝑧 ∈ π΅π‘Ÿ ,
σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©(Φπœ€ 𝑧) (𝑑) − (Φπœ†,𝛿
σ΅„© 󳨀→ 0 as πœ† 󳨀→ 0+ , 𝛿 󳨀→ 0+ .
πœ€ 𝑧) (𝑑)σ΅„©
σ΅„©
σ΅„©
(34)
Therefore, there are relatively compact sets arbitrary close to
the set {(Φπœ€ 𝑧)(𝑑) : 𝑧 ∈ π΅π‘Ÿ }; hence, the set {(Φπœ€ 𝑧)(𝑑) : 𝑧 ∈ π΅π‘Ÿ }
is also precompact in 𝑋.
4. Main Results
Consider the following linear fractional differential system:
𝐷𝑑𝛼 𝐸π‘₯ (𝑑) = 𝐴π‘₯ (𝑑) + 𝐡𝑒 (𝑑) ,
π‘₯ (0) = π‘₯0 .
𝑑 ∈ (0, 𝑏] ,
(35)
(36)
6
Abstract and Applied Analysis
It is convenient at this point to introduce the controllability
and resolvent operators associated with (35) as
Proof. Let π‘₯πœ€ be a fixed point of Φπœ€ in π΅π‘Ÿ(πœ€) . Then π‘₯πœ€ is a mild
solution of (1) on [0, 𝑏] under the control
−1
𝑏
𝐿𝑏0 = ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝐡𝑒 (𝑠) 𝑑𝑠 : 𝐿2 ([0, 𝑏] , π‘ˆ) 󳨀→ 𝑋,
π‘’πœ€ (𝑑, π‘₯πœ€ ) = (𝑏 − 𝑑)𝛼−1 𝐡∗ T∗𝐸 (𝑏 − 𝑑) 𝐽 ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯πœ€ )) ,
𝑝 (π‘₯πœ€ ) = β„Ž − S𝐸 (𝑏) π‘₯0
0
∗
𝑏
𝑏
Γ0𝑏 = 𝐿𝑏0 (𝐿𝑏0 ) = ∫ (𝑏 − 𝑠)2(𝛼−1) T𝐸 (𝑏 − 𝑠)
− ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝑓 (𝑠, π‘₯πœ€ (𝑠)) 𝑑𝑠
0
× π΅π΅∗ T∗𝐸 (𝑏 − 𝑠) 𝑑𝑠 : 𝑋 󳨀→ 𝑋,
0
(37)
respectively, where 𝐡∗ denotes the adjoint of 𝐡 and T∗𝛼 (𝑑) is
the adjoint of T𝛼 (𝑑). It is straightforward that the operator 𝐿𝑏0
is a linear bounded operator for 1/2 < 𝛼 ≤ 1.
(40)
and satisfies the following equality:
𝑏
π‘₯πœ€ (𝑏) = S𝐸 (𝑏) π‘₯0 + ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠)
0
× [π΅π‘’πœ€ (𝑠, π‘₯πœ€ ) + 𝑓 (𝑠, π‘₯πœ€ (𝑠))] 𝑑𝑠
−1
= S𝐸 (𝑏) π‘₯0 + (−πœ€πΌ + πœ€πΌ + Γ0𝑏 𝐽) ((πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯πœ€ ))
Theorem 10 (see [27]). The following three conditions are
equivalent.
𝑏
∗
∗
+ ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝑓 (𝑠, π‘₯πœ€ (𝑠)) 𝑑𝑠
∗
(i) Γ is positive; that is, βŸ¨π‘§ , Γ𝑧 ⟩ > 0 for all nonzero 𝑧 ∈
𝑋∗ .
(ii) For all β„Ž ∈ 𝑋, 𝐽(π‘§πœ€ (β„Ž)) converges to zero as πœ€ → 0+ in
the weak topology, where π‘§πœ€ (β„Ž) = πœ€(πœ€πΌ + Γ𝐽)−1 (β„Ž) is a
solution of (13).
(iii) For all β„Ž ∈ 𝑋, π‘§πœ€ (β„Ž) = πœ€(πœ€πΌ + Γ𝐽)−1 (β„Ž) converges to zero
as πœ€ → 0+ in the strong topology.
Remark 11. It is known that Theorem 10 (i) holds if and only if
Im 𝐿𝑏0 = 𝑋. In other words, Theorem 10 (i) holds if and only if
the corresponding linear system is approximately controllable
on [0, 𝑏]. Consequently, assumption (H6) is equivalent to the
approximate controllability of the linear system (35).
Theorem 12 (see [27]). Let 𝑝 : 𝑋 → 𝑋 be a nonlinear
operator. Assume that π‘§πœ€ is a solution of the following equation:
πœ€π‘§πœ€ + Γ0𝑇 𝐽 (π‘§πœ€ ) = πœ€π‘ (π‘§πœ€ ) ,
σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝑝 (π‘§πœ€ ) − π‘žσ΅„©σ΅„©σ΅„© 󳨀→ 0
as πœ€ 󳨀→ 0+ , π‘ž ∈ 𝑋.
(38)
Then there exists a subsequence of the sequence {π‘§πœ€ } strongly
converging to zero as πœ€ → 0+ .
We are now in a position to state and prove the main result
of the paper.
Theorem 13. Let 1/2 < 𝛼 ≤ 1. Suppose that conditions (S1)–
(S3), (H4)–(H5) are satisfied. Besides, assume additionally that
there exists 𝑁 ∈ 𝐿∞ ([0, 𝑏], [0, +∞)) such that
σ΅„©
σ΅„©
sup 󡄩󡄩󡄩𝑓 (𝑑, π‘₯)σ΅„©σ΅„©σ΅„© ≤ 𝑁 (𝑑) ,
π‘₯∈𝑋
for a.e. 𝑑 ∈ [0, 𝑏] .
(39)
Then system (1) is approximately controllable on [0, 𝑏].
0
−1
= β„Ž − πœ€(πœ€πΌ + Γ0𝑏 𝐽) 𝑝 (π‘₯πœ€ ) .
(41)
In other words, π‘§πœ€ = β„Ž − π‘₯πœ€ (𝑏) is a solution of
(πœ€πΌ + Γ0𝑏 𝐽) (π‘§πœ€ ) = πœ€π‘ (π‘₯πœ€ ) .
(42)
By our assumption,
𝑏
𝑇
σ΅„©2
σ΅„©
∫ 󡄩󡄩󡄩𝑓 (𝑠, π‘₯πœ€ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠 ≤ ∫ 𝑁2 (𝑠) 𝑑𝑠.
0
0
(43)
Consequently, the sequence {𝑓(⋅, π‘₯πœ€ (⋅))} is bounded. Then
there is a subsequence still denoted by {𝑓(⋅, π‘₯πœ€ (⋅))} and weakly
converges to, say, 𝑓(⋅) in 𝐿2 ([0, 𝑏], 𝑋). Then
σ΅„©
σ΅„©σ΅„©
πœ€
󡄩󡄩𝑝 (π‘₯ ) − π‘žσ΅„©σ΅„©σ΅„©
σ΅„©σ΅„© 𝑏
σ΅„©σ΅„©
σ΅„©
σ΅„©
= σ΅„©σ΅„©σ΅„©σ΅„©∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) [𝑓 (𝑠, π‘₯πœ€ (𝑠)) − 𝑓 (𝑠)] 𝑑𝑠󡄩󡄩󡄩󡄩
σ΅„©σ΅„© 0
σ΅„©σ΅„©
(44)
σ΅„©σ΅„©σ΅„© 𝑑
≤ sup σ΅„©σ΅„©σ΅„©∫ (𝑑 − 𝑠)𝛼−1 T𝐸 (𝑑 − 𝑠)
σ΅„© 0
0≤𝑑≤𝑏 σ΅„©
σ΅„©σ΅„©
σ΅„©
× [𝑓 (𝑠, π‘₯πœ€ (𝑠)) − 𝑓 (𝑠)] 𝑑𝑠󡄩󡄩󡄩 󳨀→ 0,
σ΅„©σ΅„©
where
𝑏
π‘ž = β„Ž − S𝐸 𝐸π‘₯0 − ∫ (𝑏 − 𝑠)𝛼−1 T𝐸 (𝑏 − 𝑠) 𝑓 (𝑠) 𝑑𝑠
0
(45)
as πœ€ → 0+ because of the compactness of an operator 𝑓(⋅) →
⋅
∫0 (⋅ − 𝑠)𝛼−1 T𝐸 (⋅ − 𝑠)𝑓(𝑠)𝑑𝑠 : 𝐿 2 ([0, 𝑏], 𝑋) → 𝐢 ([0, 𝑏], 𝑋).
Then by Theorem 12 for any β„Ž ∈ 𝑋,
σ΅„©σ΅„© πœ€
σ΅„© σ΅„© σ΅„©
(46)
σ΅„©σ΅„©π‘₯ (𝑏) − β„Žσ΅„©σ΅„©σ΅„© = σ΅„©σ΅„©σ΅„©π‘§πœ€ σ΅„©σ΅„©σ΅„© 󳨀→ 0
as πœ€ → 0+ . This gives the approximate controllability. The
theorem is proved.
Abstract and Applied Analysis
7
∞
Remark 14. Theorem 13 assumes that the operator 𝐸−1 is
compact and, consequently, the associated linear control
system (35) is not exactly controllable. Therefore, Theorem 13
has no analogue for the concept of exact controllability.
× ∫ πœƒπœ‰3/4 (πœƒ) exp (
0
× βŸ¨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛
∞
1 1/4
𝑑
2
𝑛=1 𝑛
Remark 15. In order to describe various real-world problems in physical and engineering sciences subject to abrupt
changes at certain instants during the evolution process,
fractional impulsive differential equations have been used
for the system model. Our result can be extended to study
the complete and approximate controllability of nonlinear
fractional impulsive differential equations of Sobolev type;
see [35, 36].
= −∑
∞
× ∫ πœ‰3/4 (πœƒ)
0
𝑏
Γ0𝑏 = ∫ (𝑏 − 𝑠)2(𝛼−1) T (𝑏 − 𝑠) T (𝑏 − 𝑠) 𝑑𝑠
0
𝑏
Example 16. Let 𝑋 = π‘ˆ = 𝐿2 [0, πœ‹]. Consider the following
fractional partial differential equation with control:
= ∫ 𝑠2(𝛼−1) T (𝑠) T (𝑠) 𝑑𝑠
0
𝑏
3 ∞
= ∫ 𝑠2(𝛼−1) ∫ 𝐸−1 πœƒπœ‰3/4 (πœƒ) 𝑆 (𝑠3/4 πœƒ) π‘‘πœƒ
4 0
0
𝐷𝑑3/4 (π‘₯ (𝑑, πœƒ) − π‘₯πœƒπœƒ (𝑑, πœƒ))
= π‘₯πœƒπœƒ (𝑑, πœƒ) + 𝑔 (𝑑, π‘₯ (𝑑, πœƒ)) + 𝑒 (𝑑, πœƒ) ,
π‘₯ (𝑑, 0) = π‘₯ (𝑑, πœ‹) = 0,
(47)
Define 𝐴 : 𝐷(𝐴) ⊂ 𝑋 → 𝑋 by 𝐴 := π‘₯πœƒπœƒ and 𝐸 :
𝐷(𝐸) ⊂ 𝑋 → 𝑋 by 𝐸π‘₯ := π‘₯ − π‘₯πœƒπœƒ , where each domain,
𝐷(𝐴) and 𝐷(𝐸), is given by
{π‘₯ ∈ 𝑋 : π‘₯, π‘₯πœƒ are absolutely continuous,
π‘₯πœƒπœƒ ∈ 𝑋, π‘₯ (𝑑, 0) = π‘₯ (𝑑, πœ‹) = 0} .
(48)
∞
∞
⟨Γ0𝑏 π‘₯, π‘₯⟩
(49)
respectively, where 𝑒𝑛 (πœƒ) := √2/πœ‹ sin π‘›πœƒ, 𝑛 = 1, 2, . . ., is the
orthonormal set of eigenvalues of 𝐴. Moreover, for any π‘₯ ∈ 𝑋,
we have
1
⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
2
𝑛=1 1 + 𝑛
∞
−𝑛2
⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
2
𝑛=1 1 + 𝑛
2
𝑛=1
(51)
Then
1
9
16 (1 + 𝑛2 )2
𝑏
∞
0
0
× ∫ 𝑠2(𝛼−1) (∫ πœƒπœ‰3/4 (πœƒ) exp (
−𝑛2
𝑆 (𝑑) π‘₯ = ∑ exp (
𝑑) ⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
1 + 𝑛2
𝑛=1
3∞ 1
∑
4 𝑛=1 1 + 𝑛2
0
∞
∞
T𝐸 (𝑑) π‘₯ =
0
2
−𝑛2 3/4
𝑠 πœƒ) π‘‘πœƒ) 𝑑𝑠
1 + 𝑛2
β©Ύ 𝛾 ∑ ⟨π‘₯, 𝑒𝑛 ⟩ .
𝐴𝐸−1 π‘₯ = ∑
3 ∞ −1
∫ 𝐸 πœƒπœ‰3/4 (πœƒ) 𝑆 (𝑑3/4 πœƒ) π‘‘πœƒ,
4 0
∞
2
𝑛=1
∞
𝑏
× βŸ¨π‘₯, 𝑒𝑛 ⟩
π‘₯ ∈ 𝐷(𝐸) ,
𝐸−1 π‘₯ = ∑
9 ∞
1
∑
16 𝑛=1 (1 + 𝑛2 )2
× ∫ 𝑠2(𝛼−1) (∫ πœƒπœ‰3/4 (πœƒ) exp (
π‘₯ ∈ 𝐷(𝐴) ,
𝑛=1
𝐸π‘₯ = ∑ (1 + 𝑛2 ) ⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
It is clear that 𝐸−1 is compact. The linear system corresponding to (47) is completely controllable if and only if there exists
𝛾 > 0 such that ⟨Γ0𝑏 π‘₯, π‘₯⟩ ≥ 𝛾‖π‘₯β€–2 for all π‘₯ ∈ 𝑋. Assume
=
𝐴 and 𝐸 can be written as follows:
𝐴π‘₯ := ∑ − 𝑛2 ⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
3 ∞ −1
∫ 𝐸 πœƒπœ‰3/4 (πœƒ) 𝑆 (𝑠3/4 πœƒ) π‘‘πœƒ 𝑑𝑠.
4 0
×
(50)
π‘₯ (0, πœƒ) = πœ™ (πœƒ) , : 0 ≤ 𝑑 ≤ 𝑏, : 0 ≤ πœƒ ≤ πœ‹.
T𝐸 (𝑑) =
𝑑
−𝑛2 3/4
𝑑 πœƒ) π‘‘πœƒ
exp (
𝑑𝑑
1 + 𝑛2
× βŸ¨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 ,
5. Applications
𝑐
−𝑛2 3/4
𝑑 πœƒ) π‘‘πœƒ
1 + 𝑛2
2
−𝑛2 3/4
𝑠 πœƒ) π‘‘πœƒ) 𝑑𝑠
1 + 𝑛2
β©Ύ 𝛾,
𝛾≤
1
9
16 (1 + 𝑛2 )2
𝑏
∞
0
0
× ∫ 𝑠−1/2 (∫ πœƒπœ‰3/4 (πœƒ) exp (
2
−𝑛2 3/4
𝑠 πœƒ) π‘‘πœƒ) 𝑑𝑠
1 + 𝑛2
8
Abstract and Applied Analysis
≤
1
9
16 (1 + 𝑛2 )2
𝑏
∞
0
0
2
× ∫ 𝑠−1/2 (∫ πœƒπœ‰3/4 (πœƒ) π‘‘πœƒ) 𝑑𝑠 󳨀→ 0,
as 𝑛 󳨀→ ∞, 󳨐⇒ 𝛾 = 0 (contradiction) ,
(52)
and no such 𝛾 > 0 exists which satisfies (51), and hence
the linear system corresponding to (47) is never completely
controllable. We show that the associated linear system is
approximately controllable on [0, 𝑏]. We need to show that
(𝑏 − 𝑠)𝛼−1 𝐡∗ T∗𝐸 (𝑏 − 𝑠)π‘₯ = 0, 0 ≤ 𝑠 < 𝑏 ⇒ π‘₯ = 0. Indeed,
(𝑏 − 𝑠)𝛼−1 𝐡∗ T∗𝐸 (𝑏 − 𝑠) π‘₯
∞
3 ∞
1
−𝑛2 3/4
exp
(
𝑠 πœƒ)
= (𝑏 − 𝑠)𝛼−1 ∫ πœƒπœ‰3/4 (πœƒ) ∑
2
4 0
1 + 𝑛2
𝑛=1 1 + 𝑛
× βŸ¨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 = 0,
∞
3 ∞
1
−𝑛2 3/4
exp
(
𝑠 πœƒ) ⟨π‘₯, 𝑒𝑛 ⟩ 𝑒𝑛 = 0,
∫ πœƒπœ‰3/4 (πœƒ) ∑
2
4 0
1 + 𝑛2
𝑛=1 1 + 𝑛
⟨π‘₯, 𝑒𝑛 ⟩ = 0 󳨐⇒ π‘₯ = 0.
(53)
Next, we suppose
(H6) 𝑔 : [0, 𝑏] × π‘… → 𝑅. For each π‘₯ ∈ 𝑅, 𝑔(⋅, π‘₯)
is measurable and for each 𝑑 ∈ [0, 𝑏], 𝑔(𝑑, ⋅) is continuous.
Moreover, supπ‘₯∈𝑅 ‖𝑔(𝑑, π‘₯)β€– ≤ 𝑁(𝑑), for a.e. 𝑑 ∈ [0, 𝑏].
Define 𝑓 : [0, 𝑏] × π‘‹ → 𝑋 by 𝑓(𝑑, π‘₯)(πœƒ) = 𝑔(𝑑, π‘₯(𝑑, πœƒ)).
Now, system (47) can be written in the abstract form (1).
Clearly, all the assumptions in Theorem 13 are satisfied if
(H6) holds. Then system (47) is approximately controllable
on [0, 𝑏].
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Discrete Dynamics in
Nature and Society
Volume 2014
Volume 2014
Journal of
Journal of
Discrete Mathematics
Journal of
Volume 2014
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Applied Mathematics
Journal of
Function Spaces
Hindawi Publishing Corporation
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Volume 2014
Hindawi Publishing Corporation
http://www.hindawi.com
Volume 2014
Hindawi Publishing Corporation
http://www.hindawi.com
Volume 2014
Optimization
Hindawi Publishing Corporation
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Volume 2014
Hindawi Publishing Corporation
http://www.hindawi.com
Volume 2014
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