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andJen-ChihYao ValeriObukhovskii MikhailKamenskii ONSOMETOPOLOGICALMETHODSINTHEORYOFNEUTRALTYPEOPERATORDIFFERENTIALINCLUSIONSWITHAPPLICATIONSTOCONTROLSYSTEMS ( 2013 ) 193–204doi:10.7151/dmdico.1152 DiscussionesMathematicaeDifferentialInclusions,ControlandO

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doi:10.7151/dmdico.1152

ON SOME TOPOLOGICAL METHODS IN THEORY OF NEUTRAL TYPE OPERATOR DIFFERENTIAL INCLUSIONS WITH APPLICATIONS TO CONTROL

SYSTEMS

Mikhail Kamenskii Faculty of Mathematics Voronezh State University

394006 Voronezh, Russia e-mail: mikhailkamenski@mail.ru

Valeri Obukhovskii 1,2 Faculty of Physics and Mathematics Voronezh State Pedagogical University

394043 Voronezh, Russia e-mail: valerio-ob2000@mail.ru

and Jen-Chih Yao Center for Fundamental Science

Kaohsiung Medical University Kaohsiung 807, Taiwan

and

Department of Mathematics King Abdulaziz University

P.O. Box 80203, Jeddah 21589, Saudi Arabia e-mail: yaojc@kmu.edu.tw

Abstract

We consider a neutral type operator differential inclusion and apply the topological degree theory for condensing multivalued maps to justify the question of existence of its periodic solution. By using the averaging method,

1

The corresponding author.

2

This research was partially supported by the Russian FBR Grants 13-01-00041 and 14-01-

00468.

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we apply the abstract result to an inclusion with a small parameter. As example, we consider a delay control system with the distributed control.

Keywords: operator differential inclusion, neutral type, periodic solution, fixed point, multivalued map, condensing map, topological degree, averaging method, control system, distributed control.

2010 Mathematics Subject Classification: Primary: 34K09; Secondary:

34C29, 34K13, 34K35, 34K40, 47H05, 47H08, 47H11.

1. Introduction

In this paper, we study the existence of periodic solutions for a neutral type operator differential inclusion of the form

˙

x ∈ F (x, ˙ x).

It is shown that under appropriate conditions this problem may be reduced to the existence of a fixed point for a condensing multivalued operator and the general existence principle (Theorem 3) can be formulated in terms of the topological degree theory for condensing multifields (see [1, 5]). As an example of applica- tion of this general principle, we consider, by using the averaging method, the solvability of a neutral type operator differential inclusion with a small parameter (Theorem 4). In the last section of the paper we present an example showing how the periodic problem for a system with the distributed control governed by the delay functional differential equation of neutral type can be reduced to the above inclusion.

2. Preliminaries

We describe some notions of the theory of multivalued maps that will be used in the sequel (details can be found, e.g., in [1]–[5]).

Let (X, d X ) and (Z, d Z ) be metric spaces. By the symbols K(Z) we denote the collection of all nonempty compact subsets of Z. If Z is a normed space, the symbol Kv(Z) denotes the collection of all nonempty compact convex subsets of Z.

Definition 1. A multivalued map (multimap) Φ : X → K(Z) is said to be

upper semicontinuous (u.s.c.) at a point x 0 ∈ X if for every ε > 0 there exists

δ > 0 such that d X (x 0 , x) < δ implies Φ(x) ⊂ V ε (Φ(x 0 )), where V ε denotes the

ε-neighborhood of a set. If Φ is u.s.c. at each point x ∈ X, it is called u.s.c.

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Definition 2. A u.s.c. multimap Φ : X → K(Z) is completely u.s.c. if its restriction on each bounded subset Ω ⊂ X is compact, i.e., the set Φ(Ω) is relatively compact in Z.

Let us mention the following useful fact (see, e.g., [2]–[5]).

Proposition 1. If a multimap F : X → K(Y ) is u.s.c. and M ⊂ X is a compact set, then the set F (M ) is compact in Y.

Definition 3. A real-valued function χ that assigns to each bounded set Ω ⊂ X the number

χ(Ω) = inf{ > 0 : Ω has a finite  − net}

is called the Hausdorff measure of noncompactness (MNC) in X.

In the sequel we will need the following assertion.

Lemma 1. Let (X, d) be a metric space and Z a normed space; A ⊆ X a closed subset; a multimap G : A × X → K(Z) satisfies the following conditions:

(G1) for each y ∈ X, the multimap G(·, y) : A → K(Z) is completely u.s.c.;

(G2) for each x ∈ A, the multimap G(x, ·) : X → K(Z) is k-Lipschitz w.r.t. the Hausdorff metric h on K(Z), where k ≥ 0, i.e.,

h G(x, y), G(x, y 0 ) ≤ kd(y, y 0 )

for all y, y 0 ∈ X.

Then the multimap H : A → K(Z), H(x) = G(x, x) is u.s.c. and (k, χ 0 , χ 1 )- bounded, where χ 0 and χ 1 are the Hausdorff MNCs in X and Z respectively, i.e.,

χ 1 (H(Ω)) ≤ kχ 0 (Ω) for each bounded set Ω ⊆ A.

Proof. Take any point (x 0 , y 0 ) ∈ A × X and fix ε > 0. Denote by B r an open ball in Z of radius r > 0 centered at the origin. Take convergent sequences {x n } ⊂ A and {y n } ⊂ X : x n → x 0 and y n → y 0 . Suppose that an integer N is such that for all n ≥ N :

(i) d(y n , y 0 ) ≤ 2k ε ;

(ii) G(x n , y 0 ) ⊂ G(x 0 , y 0 ) + 2 ε B 1 .

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From condition (G2) it follows that for n ≥ N we have

G(x n , y n ) ⊂ G(x n , y 0 ) + kB d(y

n

,y

0

) ⊂ G(x n , y 0 ) + ε 2 B 1 . Applying (ii), we obtain

G(x n , y n ) ⊂ G(x 0 , y 0 ) + εB 1

for n ≥ N , demonstrating that G is u.s.c. at (x 0 , y 0 ), the conclusion that H is u.s.c. immediately follows.

The fact that the multimap H is (k, χ 0 , χ 1 )-bounded, can be proved in the same way as Proposition 2.2.2 in [5].

Now, suppose that U is an open bounded subset in a Banach space E , its closure is denoted as U and ∂U denotes its boundary. Let Φ : U → Kv(E ) be a u.s.c.

multimap such that

F ixΦ ∩ ∂U = ∅,

where F ixΦ = {x : x ∈ Φ(x)} is the fixed point set. If Φ is k-condensing, 0 ≤ k < 1, w.r.t. the Hausdorff MNC χ E , i.e.,

χ E (Φ(Ω)) ≤ kχ E (Ω)

for each Ω ⊂ U , then the topological degree deg(i − Φ, U ) of the corresponding multivalued vector field (multifield) Ψ = i − Φ, Ψ(x) = x − Φ(x) is well defined and satisfies all usual properties. Let us mention some of them.

1) Fixed point property. If deg(i−Φ, U ) 6= 0, then F ixΦ is a nonempty compact subset of U.

2) Map restriction property. If E 0 is a closed subspace of E and Φ(U ) ⊂ E 0 , then

deg(i − Φ, U ) = deg E

0

(i − Φ, U ∩ E 0 ), where deg E

0

denotes the degree evaluated in the subspace E 0 .

3) Homotopy invariance property. If Υ : U × [0, 1] → Kv(E ) is a family of k-condensing multimaps in the sense that

χ E (Υ(Ω × [0, 1])) ≤ kχ E (Ω)

for each Ω ⊂ U , and F ixΥ(·, λ) ∩ ∂U = ∅ for all λ ∈ [0, 1], then

deg(i − Υ(·, 0), U ) = deg(i − Υ(·, 1), U ).

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As the corollary of the last property, we can consider the following assertion.

Proposition 2. Suppose that u.s.c. k-condensing multimaps Φ 0 , Φ 1 : U → Kv(E ) satisfy the following boundary condition: for each x ∈ ∂U , the sets Ψ 0 (x) = x − Φ 0 (x) and Ψ 1 (x) = x − Φ 1 (x) do not contain the vectors which have opposite directions, i.e.,

y 0

ky 0 k 6= − y 1

ky 1 k for all y 0 ∈ Ψ 0 (x), y 1 ∈ Ψ 1 (x).

Then

deg(i − Φ 0 , U ) = deg(i − Φ 1 , U ).

3. General existence principle

For a given T > 0, by C T and L p T we will denote, respectively, the space of T −periodic continuous functions x : R → R n and the space of T −periodic p−integrable functions y : R → R n (p > 1) with norms:

kxk C = sup t∈[0,T ] kx(t)k and

kyk L

p

=  Z T 0

ky(s)k p ds 

1p

.

We will consider the neutral type operator differential inclusion of the following form

(3.1) x ∈ F (x, ˙ ˙ x),

where the multimap F : C T × L p T → Kv(L p T ) satisfies the following conditions:

F 1) for each y ∈ L p T , the multimap F (·, y) : C T → Kv(L p T ) is u.s.c.;

F 2) for each x ∈ C T , the multimap F (x, ·) : L p T → Kv(L p T ) is k−Lipschitz with respect to the Hausdorff metric h on Kv(L p T ) with 0 ≤ k < 1, i.e.,

(3.2) h F (x, y 0 ), F (x, y 1 ) ≤ kky 0 − y 1 k L

p

for all y 0 , y 1 ∈ L p T .

By a solution of problem (3.1) we mean a function x belonging to the Sobolev

space H T 1,p of T -periodic functions satisfying inclusion (3.1).

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Let us demonstrate that problem (3.1) can be reduced to a fixed point problem for an appropriate multimap. Denote Y = R n × L p T and define the multimap Φ : Y → Kv(Y) as

(3.3) Φ(λ, v) = Φ 0 (λ, v), Φ 1 (λ, v), where

Φ 0 (λ, v) = λ + m(v) with

m(v) = 1 T

Z T 0

v(s)ds and

Φ 1 (λ, v) = F (λ + J v, v) with

(J v)(t) = Z t

0

v(s)ds − tm(v).

The multimap Φ is said to be associated with inclusion (3.1).

One can verify the following assertion.

Proposition 3. If a function x ∈ H T 1,p is a solution of problem (3.1), then (x(0), ˙ x) ∈ F ixΦ. Conversely, if (λ, v) ∈ F ixΦ, then x = λ + J v is the solution of (3.1).

Let the space Y be endowed with the following norm:

k(λ, v)k Y = max kλk R

n

, kvk L

p

T

.

The corresponding Hausdorff MNC in Y will be denoted by χ Y .

We will need the following auxiliary statement which can be easily verified.

Proposition 4. For each bounded set ∆ ⊂ Y we have

(3.4) χ Y (∆) = χ L (pr L (∆)),

where pr L (∆) denotes the natural projection of ∆ on L p T and χ L is the Hausdorff MNC in the space L p T .

Let us mention the next important property of the multioperator Φ.

Theorem 2. Under conditions (F 1), (F 2) the multioperator Φ is u.s.c. and

k-condensing with respect to χ Y .

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Proof. It is clear that, to prove the upper semicontinuity of Φ, it is sufficient to demonstrate the same property for the multimap Φ 1 . Consider the multimap G : Y × Y → Kv(L p T ) defined as

G (λ, v), (µ, w) = F(λ + Jv, w)

Notice that the map ψ : Y → C T , ψ(λ, v) = λ + J v transforms each bounded set ∆ ⊂ Y into a relatively compact set in C T . Then, by using Proposition 1, it is easy to see that the multimap G satisfies conditions of Lemma 2 and hence the multimap Φ 1 (λ, v) = G (λ, v), (λ, v) is u.s.c. and, moreover, applying Proposition 4, for each bounded set ∆ ⊂ Y we have:

χ Y (Φ(∆)) = χ L1 (∆)) ≤ kχ Y (∆).

As the direct consequence, it follows that we may formulate the next general existence principle for inclusion (3.1).

Theorem 3. Let the multimap F : C T × L p T → Kv(L p T ) satisfy conditions (F 1), (F 2) and there exists a bounded open set U ⊂ Y such that inclusion (3.1) has no solutions x(·) such that (x(0), ˙ x) ∈ ∂U and

deg(i − Φ, U ) 6= 0.

Then inclusion (3.1) has a solution x(·) such that (x(0), ˙ x) ∈ U.

We will demonstrate the application of this principle to the solvability of the following parametrized inclusion

(3.5) x ∈ εF (x, ˙ ˙ x),

where the multimap F satisfies conditions (F 1), (F 2) and the parameter ε > 0 is sufficiently small.

Towards this goal, introduce the multioperator F 0 : R n → Kv(R n ) defined in the following way

(3.6) F 0 (λ) = 1 T

Z T 0

F (λ, 0)(s)ds :=  1 T

Z T 0

f (s)ds : f ∈ F (λ, 0)

 , where λ ∈ C T is the constant function that is equal identically to λ ∈ R n . Theorem 4. Suppose that inclusion

(3.7) 0 ∈ F 0 (λ)

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has a solution λ ∈ R n with a bounded neighborhood U (λ ) such that (3.8) 0 / ∈ F 0 (λ), ∀λ ∈ ∂U (λ )

and

(3.9) deg (−F 0 , U (λ )) 6= 0.

Then for all sufficiently small ε > 0 inclusion (3.5) has a solution x ε such that x ε (t) ∈ U (λ ) for all t ∈ [0, T ] and k ˙ x ε k L

p

→ 0 while ε → 0.

Proof. Consider the set V = U (λ ) × B L

p

T

(0, r) ⊂ Y, where r > 0 and define the multimap Γ ε : V → Kv(R n × R n ) ⊂ Kv(Y) as

Γ ε (λ, y) = (λ + m(y), m(y) + εF 0 (λ)) . Notice that for each (λ, y) ∈ ∂V we have

(λ, y) / ∈ Γ ε (λ, y).

Indeed, supposing the contrary, we will have for some (λ 0 , y 0 ) ∈ ∂V : λ 0 = λ 0 + m(y 0 ),

y 0 ∈ m(y 0 ) + εF 0 (λ 0 ).

Since y 0 is a constant function, from the first equality it follows that y 0 ≡ 0.

Hence λ 0 ∈ ∂U (λ ) and the last inclusion yields 0 ∈ εF 0 (λ 0 ).

Since ε > 0 we get

0 ∈ F 0 (λ 0 ).

contrary to assumption (3.8).

Now, let us evaluate

deg(i − Γ ε , V).

Since the image of the multimap Γ ε is contained in the space R n ×R n , by applying the map restriction property of the topological degree, we get

deg(i − Γ ε , V) = deg R

n

×R

n

(i − Γ ε , V n ),

where V n = U (λ ) × B R

n

(0, r).

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Further, considering ε as the homotopy parameter, we obtain deg R

n

×R

n

(i − Γ ε , V n ) = deg R

n

×R

n

(i − Γ 1 , V n ).

The multimap Γ 1 on V n is defined by the formula

Γ 1 (u 1 , u 2 ) = (u 1 + u 2 , u 2 + F 0 (u 1 ))

and hence the corresponding multifield i − Γ 1 on the same set has the form (i − Γ 1 ) (u 1 , u 2 ) = A (−F 0 (u 1 ), −u 2 ) ,

where A(v 1 , v 2 ) = (v 2 , v 1 ).

Applying the multiplicative property of the topological degree (see, e.g., [1, 6]), we get

deg R

n

×R

n

(i − Γ 1 , V n ) = (−1) n deg (−F 0 , U (λ )) yielding

deg(i − Γ ε , V) = (−1) n deg (−F 0 , U (λ )) 6= 0 for each ε > 0.

Let Φ ε : Y → Kv(Y) be the multimap associated with inclusion (3.5). We will show that, for sufficiently small ε > 0, the multifields i − Φ ε and i − Γ ε do not admit opposite directions on ∂V.

Supposing the contrary, we will have sequences ε k → 0, and

(3.10) (λ k , y k ) ∈ ∂V

such that the sets (λ k , y k ) − Φ εk , y k ) and (λ k , y k ) − Γ εk , y k ) contain opposite vectors. Since the first components of both sets are equal to m(y k ), we have m(y k ) = 0 for all k ≥ 1. Considering the second component, we conclude that there exists a sequence {α k } ⊂ [0, 1] such that

(3.11) y k ∈ α k ε k F (λ k + J y k , y k ) + (1 − α kk F 0k ), ∀k ≥ 1.

From Theorem 2 it follows that the set S

k F (λ k + J y k , y k ) is bounded, so there exists a constant C ≥ 0 such that

(3.12) ky k k L

p

≤ Cε k , ∀k ≥ 1.

Hence

ky k k L

p

→ 0 as k → ∞.

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Further, we can assume, w.l.o.g., that λ k → λ 0 . Passing to the limit in inclusions (3.10), we obtain

(λ 0 , 0) ∈ ∂



U (λ ) × B L

p

T

(0, r)



that yields λ 0 ∈ ∂U (λ ).

Averaging both the parts of inclusion (3.11), and dividing on ε k > 0 we get (3.13) 0 ∈ α k m (F (λ k + J y k , y k )) + (1 − α k )F 0k ), ∀k ≥ 1.

Taking into consideration that

kJ y k k C ≤ T 1−

p1

2ky k k L

p

T

→ 0 and passing to the limit in inclusion (3.13) we obtain

0 ∈ F 0 (λ 0 ) that is the contradiction.

So, applying Proposition 2, we come to the conclusion that deg(i − Φ ε , V) = deg(i − Γ ε , V) 6= 0

for each ε > 0 sufficiently small, yielding the existence of pairs (λ ε , y ε ) ∈ V satisfying

(3.14) (λ ε , y ε ) ∈ Φ εε , y ε ).

But then functions

x ε = λ ε + J (y ε ) are solutions of (3.5).

Notice that inclusions (3.14) imply the existence of a constant C 1 ≥ 0 such that

ky ε k L

p

≤ C 1 ε, yielding

k ˙x ε k L

p

= ky ε k L

p

→ 0 as ε → 0.

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4. Example: periodic control problem

Consider a periodic control system governed by the following neutral type func- tional differential equation:

(4.1) x 0 (t) = f



t, x(t − h), x 0 (t − h), 1 δ

Z t t−δ

u(s)ds

 ,

where f : R × R n × R n × R m → R n is a Carath´ eodory type function, T -periodic in the first argument, h > 0 and δ > 0 are given numbers. It is supposed that f is locally integrably bounded in the sense that for each r > 0 there exists a function ν r ∈ L p + [0, T ], p > 1 such that

kf (t, x, y, v)k ≤ ν r (t) for a.e. t ∈ [0, T ], provided kxk, kyk, kvk ≤ r.

We will assume also that f is k-Lipschitz in the third argument with 0 ≤ k < 1 :

kf (t, x, y 0 , v) − f (t, x, y 1 , v)k ≤ kky 0 − y 1 k for a.e. t ∈ [0, T ] and x, y 0 , y 1 ∈ R n ; v ∈ R m .

We will suppose that the set f (t, x, y, M ), t ∈ R; x, y ∈ R n is convex for each convex M ⊂ R m .

At last, we assume that control functions u belong to the space of periodic functions L q T (R m ), q > 1 and they fill the set of admissible controls M defined as

M = {u ∈ L q T (R m ) : u(t) ∈ V for a.e. t ∈ [0, T ]}, where V ⊂ R m is a given compact convex set.

Notice that the corresponding set N =



v : v(t) = 1 δ

Z t t−δ

u(s)ds



is compact and convex in C T (R m ).

Define the multimap F : C T × L p T ( L p T by

F (x, y) = {z ∈ L p T : z(t) = f (t, x(t − h), y(t − h), v(t)), v ∈ N}.

By using [7], page 384, one can show that each set F (x, y) is convex compact.

It is easy to verify also that the multimap F satisfies conditions (F 1) and (F 2)

of the previous section. So, the study of system (4.1) can be reduced to the

investigation of inclusion (3.1) where we can apply the topological degree theory

to its analysis.

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The authors would like to express their gratitude to the anonymous referee for his/her valuable remarks.

References

[1] Yu.G. Borisovich, B.D. Gelman, A.D. Myshkis and V.V. Obukhovskii, Topological methods in the theory of fixed points of multivalued mappings. (Russian) Uspekhi Mat. Nauk 35 (1980), 59–126. English translation: Russian Math. Surveys 35 (1980), 65–143. doi:10.1070/RM1980v035n01ABEH001548

[2] Yu.G. Borisovich, B.D. Gelman, A.D. Myshkis and V.V. Obukhovskii, Introduction to the Theory of Multivalued Maps and Differential Inclusions, (Russian) Second edition, Librokom, Moscow, 2011.

[3] L. G´ orniewicz, Topological Fixed Point Theory of Multivalued Mappings, 2nd edi- tion, Topological Fixed Point Theory and Its Applications, 4. Springer, Dordrecht, 2006.

[4] S. Hu and N.S. Papageorgiou, Handbook of Multivalued Analysis, Vol. I. Theory, Mathematics and its Applications, 419. Kluwer Academic Publishers, Dordrecht, 1997.

[5] M. Kamenskii, V. Obukhovskii and P. Zecca, Condensing Multivalued Maps and Semilinear Differential Inclusions in Banach Spaces, de Gruyter Series in Nonlinear Analysis and Applications, 7. Walter de Gruyter & Co., Berlin, 2001.

doi:10.1515/9783110870893

[6] M.A. Krasnosel’skii and P.P. Zabreiko, Geometrical Methods of Nonlinear Analysis, A Series of Comprehensive Studies in Mathematics, 263, Springer-Verlag, Berlin- Heidelberg-New York-Tokio, 1984.

[7] M.A. Krasnoselskii, P.P. Zabreiko, E.I. Pustyl’nik and P.E. Sobolevskii, Integral Operators in Spaces of Summable Functions, Noordhoff International Publishing, Leyden, 1976.

Received 7 August 2013

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