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Volume 2010, Article ID 281238,14pages doi:10.1155/2010/281238

Research Article

Approximate Controllability of

a Reaction-Diffusion System with

a Cross-Diffusion Matrix and Fractional

Derivatives on Bounded Domains

Salah Badraoui

Laboratoire LAIG, Universit´e du 08 Mai 1945, BP. 401, Guelma 24000, Algeria

Correspondence should be addressed to Salah Badraoui,[email protected]

Received 11 July 2009; Accepted 5 January 2010

Academic Editor: Ugur Abdulla

Copyrightq2010 Salah Badraoui. 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 study the following reaction-diffusion system with a cross-diffusion matrix and fractional derivativesutauavc1−Δα1uc2−Δα2vf1x, tinΩ×0, t∗,vtbubv

d1−Δβ1ud2−Δβ2vf2x, tinΩ× 0, t∗,uv0 onΩ×0, t∗,ux,0 u0x,vx,0

v0xinx∈Ω,whereΩ⊂RNN≥1is a smooth bounded domain,u0, v0∈L2Ω, the diffusion

matrixM a1a2

b1b2

has semisimple and positive eigenvalues 0 < ρ1 ≤ ρ2, 0 < α1, α2, β1, β2< 1,

ω⊂Ωis an open nonempty set, and 1ωis the characteristic function ofω. Specifically, we prove that under some conditions over the coefficientsai, bi, ci, dii1,2, the semigroup generated by the linear operator of the system is exponentially stable, and under other conditions we prove that for allt>0 the system is approximately controllable on0, t∗ .

1. Introduction

In this paper we prove controllability for the following reaction-diffusion system with cross diffusion matrix:

utauavc1−Δα1uc2−Δα2v1ωf1x, t inΩ× 0, t,

vtbubvd1−Δβ1ud2−Δβ2vf2x, t inΩ× 0, t,

uv0 onΩ× 0, t,

ux,0 u0x, vx,0 v0x inx∈Ω,

1.1

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We assume the following assumptions.

H1 Ωis a smooth bounded domain inRN N1.

H2The diffusion matrixMa1a2 b1 b2

has semisimple and positive eigenvalues 0< ρ1≤

ρ2.

H3cj, dj j 1,2are real constants,αj, βj j1,2are real constants belonging to the interval 0,1.

H4u0, v0∈L.

H5The distributed controlsf1, f2∈L20, t∗ ;L2Ω.

Specifically, we prove the following statements.

iIf c2d10 and min{c1λ11−α1ρ1, d2λ11−β2ρ1}>0, whereλ1is the first eigenvalue

of−Δwith Dirichlet condition, or if c2/0, d1/0, c1 ≥0, andd2 ≥ 0; then, under

the hypothesesH1–H3, the semigroup generated by the linear operator of the system is exponentially stable.

iiIf c2d10 and under the hypothesesH1–H5, then, for allt>0 and all open

nonempty subset ωofΩthe system is approximately controllable on 0, t.

This paper has been motivated by the work done in1 and the work done by H. Larez and H. Leiva in2 . In the work1 , the auther studies the asymptotic behavior of the solution of the system

uta 2u

∂x2 β

∂u ∂xb

2v

∂x2 ft, u, v, x∈R, t >0,

vtc 2u

∂x2 d

2v

∂x2 β

∂v

∂xgt, u, v, x∈R, t >0

1.2

supplemeted with the initial conditions

ux,0 u0x, vx,0 v0x, x∈R. 1.3

The author proved that in the Banach spaceX×X where XCubRis the space of bounded

uniformly continuous real valued functions onR, iff andg are locally Lipshitz and under some conditions over the coefficients a, b, c, d, β, and if u0, v0 ∈ C {u ∈ CubR :

limx→∞uxexist},then ut, vtC for all t < tmax.Moreover, Ut limx→∞ux andVt limx→∞vxsatisfy the system of ordinary differential equations

Ut ft, Ut, Vt,

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with the initial data

U0 lim

x→∞u0x, V0 xlim→∞v0x. 1.5

The same result holds forC−{u∈CubR: limx→ −∞uxexist}.

In the work done in2 , the authers studied the system1.1withc2d10, c1d2,

and α1 β2 1/2. They proved that if the diffusion matrix

a b

c d

has semi-simple and positive eigenvalues 0< ρ1≤ρ2,f1, f2∈L20, τ;L,then ifλ11/2ρ1β >0λ1is the first

eigenvalue of−Δ, the system is approximately controllable on 0, τ for all open nonempty subset ωofΩ.

2. Notations and Preliminaries

In the following we denote by

M2Rthe set of 2×2 matrices with entries fromR,

L2Ωthe set of all measurable functionsu:Ω Rsuch that

Ω|u|2dx <∞,

H1Ω the set of all the functions u L2Ω that have generalized derivatives

∂u/∂xjL2Ωfor allj1, . . . , N, H1

0Ωthe closure of the setC∞0 Ωin the Hilbert spaceH1Ω,

H2Ω the set of all the functions u L2Ω that have generalized derivatives

∂u/∂xj, ∂2u/∂xj∂xkL2Ωfor allj, k1, . . . , N.

We will use the following results.

Theorem 2.1cf.3 . Let us consider the following classical boundary-eigenvalue problem for the

laplacien:

−Δuλu, onΩ,

u0, on∂Ω, 2.1

whereΩis a nonempty bounded open set inRNandDΔ H2ΩH1 0Ω.

This problem has a countable system of eigenvalues 0< cλ1 < λ2 <· · · < λj < · · · and λj → ∞asj → ∞.

iAll the eigenvalues λj have finite multiplicity mj equal to the dimension of the corresponding eigenspaceSj.

iiLet{ϕjk} mj

k1be a basis of the Sjfor everyj,then the eigenvectors {ϕjk}

mj,

k1,j1form

a complete orthonormal system in the space L2Ω.Hence for all u L2Ωwe

haveuj1mj

k1u, ϕjkϕjk.If we putEju

mj

k1u, ϕjkϕjk then we get u

j1Eju.

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ivFor alluD−Δwe have −Δuj1λjEju.

vThe operatorΔgenerates an analytic semigroup {TΔt}on L2Ωdefined by

TΔtu

j1

eλjtEju. 2.2

Definition 2.2. Let 0< α <1 a real number, the operator−Δαis defined by

−Δα:DΔαL2Ω−→L2Ω,

D−Δα

⎧ ⎨

uL2Ω|

j1

mj

k1

λαju, ϕjk

2

<

⎫ ⎬ ⎭,

−Δαuj1

mj

k1

λαjϕjk, u

ϕjk.

2.3

In particular, we obtain ϕjkD−Δα and −Δαϕjk λαjϕjk. Since {ϕjk} mj,

k1,j1 form a

complete orthonormal system in the spaceL2Ω,then it is dense inL2Ω, and henceDΔα is dense in L2Ω.

Proposition 2.3cf.4 . LetXbe a Hilbert separable space and{Aj}j1and {Pj}j1two families

of bounded linear operators inX, with{Pj}j1a family of complete orthogonal projections such that AjPjPjAj, j ≥1.

Define the following family of linear operatorsStwj1eAjtP

jw, wX, t≥0.Then aStis a linear and bounded operator if eAjtgt, j1withgt0,continiuous for

t≥0,

bunder the above condition (a),{St}t0is a strongly continiuous semigroup in the Hilbert spaceX,whose infinitesimal generatorAis given by

Aw

j1

AjPjw, wDA, DA

⎧ ⎨ ⎩wX|

j1

AjPjw2

<

⎫ ⎬

. 2.4

Theorem 2.4cf.5 . SupposeΩis connected,fis a real function inΩ, andf 0on a nonempty

open subset ofΩ. Thenf≡0inΩ.

3. Abstract Formulation of the Problem

In this section we consider the following notations.

iXL2Ω×L2Ω. Xis a Hilbert space with the inner product

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iiWe define

A11u, v auavc1−Δα1uc2−Δα2v,

A12u, v bubvd1−Δβ1ud2−Δβ2v.

3.2

iiiLetw u, v,then we can define the linear operator

A:DAX−→X,

DA H2Ω;RH1 0Ω;R

2

,

AwMΔ−c1B1−Δα1c2B2−Δα2d1B3−Δβ1d2B4−Δβ2

w, 3.3 where M

a1 a2

b1 b2

, B1

1 0 0 0

, B2

0 1 0 0 , B3 0 0 1 0

, B4

0 0 0 1 . 3.4

Therefore, for allwDA

A11u, v a1

j1

λjEjua2

j1

λjEjvc1

j1

λα1j Ejuc2

j1

λα2j Ejv,

A12u, v b1

j1

λjEjub2

j1

λjEjvd1

j1

λβ1j Ejud2

j1

λβ2j Ejv.

3.5

If we put

Pj

Ej 0 0 Ej

, j1,2, 3.6

then3.3can be written as

Aw

A11u, v

A12u, v

j1

λjMλα1j c1B1λα2j c2B2λβ1j d1B3λβ2j d2B4

Pjw, 3.7

and we have for allwX

w

j1

Pjw, w2 ∞

j1

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Consequently, system1.1can be written as an abstract differential equation in the Hilbert spaceXin the following form:

w−AwBωft, inΩ× 0, t,

w0, on 0, t∗×Ω,

w0 w0, inx∈Ω,

3.9

wheref ≡colf1, f2∈L20, T ;X and

1

ω 0

0 1ω

is a bounded linear operator fromU intoX.

4. Main Results

4.1. Generation of a

C

0

-Semigroup

Theorem 4.1. Ifc2 d1 0, then, under hypotheses (H1)–(H3), the linear operator−Adefined by

3.3is the infinitesimal generator of strongly continuous semigroup{St}t0given by

Stw

j1

eAjtP

jw, wX, 4.1

where

Mj −λjMλα1j c1B1−λα2j c2B2−λβ1j d1B3−λβ2j d2B4, 4.2

AjMjPj. 4.3

Moreover, if

minc1λ11α1ρ1, d2λ11β2ρ1

>0, 4.4

then theC0-semigoup{St}t≥0is exponentially stable, that is, there exist two positives constantsc, δ such that

Stceδt, for allt≥0. 4.5

Proof. In order to apply theProposition 2.3, we observe that−Acan be written as follows:

−Aw∞ j1

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where

Aj

λjMλα1j c1B1λα2j c2B2λβ1j d1B3λβ2j d2B4

Pj. 4.7

Therefore,AjMjPjandAjPjPjAj.

Now, we have to verify condition a of theProposition 2.3. We shall suppose that 0< ρ1< ρ2.Then, there exists a set{Q1, Q2} ∈M2R 2of complementary projections onR2

such that

eMteρ1tQ

1eρ2tQ2. 4.8

IfG g11g21g12g22is the matrix passage from the canonical basis ofR2 to the basis composed

with the eigenvectors ofM, then

Q1

1 ρ1ρ2

g11g22 −g11g12

g21g22 −g12g21

, Q2

1 ρ1ρ2

−g12g21 g11g12

−g21g22 g11g22

. 4.9

Hence,

eλjMteλjρ1tQ

1eλjρ2tQ2. 4.10

We have also

eλαj1c1B1t

⎛ ⎝eλ

α1

j c1t 0

0 1

, eλα2

j c2B2t

1 −λα2j c2t

0 1

,

eλβj1d1B3t

⎝ 1 0

−λβ1 j d1t 1

, eλβ1

j d2B4t

⎛ ⎝1 0

0 eλβj2d2t

⎞ ⎠.

4.11

From4.10-4.11into4.7we obtain

eAjteλjρ1tQ

1eλjρ2tQ2

KjtPj, 4.12

where

Kjt

⎛ ⎜ ⎝e

λα1

j c1tλα2β1

j c2d1t2eλ α1

j c1t −λα2

j c2teλ α1

j c1λ β2

j d2t

−λβ1

j d1t eλ

β2

j d2t

⎞ ⎟

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Asc2d10 we get

Kjt

⎛ ⎝eλ

α1

j c1t 0

0 eλβj2d2t

. 4.14

Asλj → ∞asj → ∞,then this implies the existence of a positive numbercand a real number δ such that eAjtceδt, for every j1.Therefore−Ais a strongly continious

semigroup{St}t0given by4.1. We can even estimate the constantscandδas follows. i If min{c1 λ11α1ρ1, d2 λ11−β2ρ1} ≤ 0. As limj→ ∞{−λα1j c1 λ

1−α1

j ρ1} limj→ ∞{−λβ2j c1λj1−β2ρ1}−∞, then there exist constants

δ1max

−λα1 j

c1λ1jα1ρ1

|λα1j c1λ1jα1ρ1

≤0, j ≥1,

δ2max

−λβ2 j

d2λ1jβ2ρ1

|λβ2j d2λ1jβ2ρ1

≤0, j ≥1,

4.15

hence, if we put

δmax{δ1, δ2} ≥0, 4.16

c0

1 ρ1ρ2 max

g11g22,g11g12,g21g22,g12g21, 4.17

we easily obtain

eAjt4c

0eδt, j≥1. 4.18

iiIf min{c1λ11α1ρ1, d2λ11β2ρ1}>0. If we put

δminλα11c1λ11α1ρ1

, λβ21 d2λ11β2ρ1

>0, 4.19

then we find that

eAjt4c

0eδt, j≥1. 4.20

Therefore, the linear operator−Agenerates a strongly continuous semigroup{St}t0 onX given by expression4.1.

Finally, if min{c1 λ11−α1ρ1, d2 λ11−β2ρ1} > 0,we have already proved 4.20. Using

4.20into4.1we get that theC0-semigoup{St}t≥0is exponentially stable. The expression

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Theorem 4.2. If

c2/0, d1/0, c1≥0, d2≥0, 4.21

then, under the hypotheses (H1)–(H3), the linear operator−A defined by3.3 is the infinitesimal generator of strongly continuous semigroup exponentially stable{St}t0defined by4.1. Specially, there exist two positives constantsc, δsuch that

Stceδt, ∀t≥0. 4.22

To prove this result, we need the following lemma.

Lemma 4.3. For every two real positives constantscandλ, one has for every0< δ < λ/c

cteλt≤ 1 eλ/cδe

δct, ∀t0, 4.23

and for every0< δ < λ/c

ct2eλt ≤ 4

e2λ/cδe

δct, ∀t0. 4.24

Proof ofLemma 4.3.It is easy to verify that for every ε >0 :teεt 1/eε, for allt0. Let 0< δ < λ/candελ/cδ >0, then we get

teλ/ct≤ 1 eλ/cδe

δt, ∀t0. 4.25

Hence, we get4.23.

Also, it is easy to verify that for every ε > 0 : t2eεt 4/e2ε2, for all t 0. Let

0< δ < λ/candελ/cδ >0, then we get

t2eλct≤ 4

e2λ/cδ2e

δt, ∀t0.

4.26

Hence, from 4.26we get ct2eλtct2eλ/cct 4/e2λ/cδ2eδctfor allt 0 and 0< δ < λ/c, which gives4.24.

With the same manner we can prove that for every 0< δ < λc−1/nand every nN∗ we have

tneλc−1/ntn n

eεne

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and consequently, for every two real positives constantscandλand every n∈N∗we have

ctneλtn n

eεneδc−1/nt

, for allt≥0 and every 0< δ < λ. 4.28

Now, we are ready to proveTheorem 4.2.

Proof ofTheorem 4.2. By applyingProposition 2.3we start from formula4.12and we put

Kjt

K11,jt K12,jt

K21,jt K22,,jt

, 4.29

where

K11,jt eλ

α1

j c1tλα2β1

j c2d1t

2eλα1

j c1t, K

12,jt −λα2j c2teλ α1

j c1λ β2

j d2t,

K21,jt −λβ1j d1t, K22,,jt eλ

β2

j d2t, ∀j≥1.

4.30

To estimateeλjρ1tK

11,jtwe have in taking into accountc1 ≥0

eλjρ1λαj1c1teλ1ρ1t, ∀t≥0, 4.31

and applying theLemma 4.3jα2β1|c2d1|we get

λα2j β1c2d1t2eλjρ1λ α1 j c1t

≤ 4

e2λ1−α2β1/2

j /

|c2d1|

ρ1

λjα1α2β1/2/|c2d1|

c1−γ1

eγ1λαj2β1/2 √

|c2d1|t,

4.32

for allt ≥ 0 and 0 < γ1 < λj1−α2β1/2/

|c2d1|ρ1 λjα1α2β1/2/

|c2d1|c1. But we have

λj1−α2β1/2/|c2d1|ρ1λjα1α2β1/2/

|c2d1|c1≥λ11−α2β1/2/

|c2d1|ρ1, for allj≥1.Then

we get for every 0< γ111−α2β1/2/

|c2d1|ρ1that

λα2j β1c2d1t2eλjρ1λ α1 j c1t

≤ 4

e2λ1−α2β1/2

1 /

|c2d1|

ρ1−δ1

eγ1λ1α2β1/2 √

|c2d1|t, ∀t0. 4.33

From4.31-4.33we get

eλjρ1tK

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where

σ114

λ11α2β1/2

|c2d1|

ρ1−δ1

⎞ ⎠

−1

, δ1min λ1ρ1, γ1λ1α2β1/2

!

|c2d1|

"

, 4.35

and 0< γ1 11−α2β1/2/

|c2d1|ρ1.

ApplyingLemma 4.3and taking into account4.21we get with the same manner that for every 0< δ211α2/|c2|ρ1

eλjρ1tK

12,jtσ2eδ2λ α2

1 |c2|t, ∀t≥0, j≥1, 4.36

where

σ2

1 11α2/|c2|

ρ1−δ2

, 4.37

and or every 0< δ311β1/|d1|ρ1

eλjρ1tK

21,jtσ3eδ3λ β1

1 |d1|t, ∀t≥0, j≥1, 4.38

where

σ3

1 11β1/|d1|

ρ1−δ3

, 4.39

eλjρ1tK

22,jteλ1ρ1t, ∀t≥0, j ≥1. 4.40

From4.34-4.40into4.12we get

eAjt4c

0σeδt, ∀t≥0, j ≥1, 4.41

where c0is defined by4.17and

σ1σ1σ2σ3, 0< δ <min

δ1, δ2λα21 |c2|, δ3λβ11|d1|, λ1ρ1

. 4.42

Using4.41into4.1we get that theC0-semigoup{St}t≥0generated by−Ais exponentially

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4.2. Approximate Controllability

Befor giving the definition of the approximate controllabiliy for the sytem3.9, we have the following known result: for allw0 ∈XandfL2 0, T;U,the initial value problem3.9

admits a unique mild solution given by

wt Stw0

#t

0

StτBωfτdτ, t∈0, T . 4.43

This solution is denoted bywt;f.

Definition 4.4. System3.9is said to beapproximately controllableat timet∗whenever the set Ft∗{wt∗;f| ∀f ∈L2 0, t∗;U}is densely embedded inX; that is,

∀w0, w1 ∈X, ∀ε >0; ∃f∈L2 0, t∗;U:w

t∗;fw1< ε. 4.44

The following criteria for approximate controllability can be found in6 .

Criteria 1. System3.9is approximately controllable on0, t∗ if and only if

BStw0, ∀t∈0, t∗ ⇒w0. 4.45

Now, we are ready to formulate the third main result of this work.

Theorem 4.5. If the following condition

c2d10 4.46

is satisfied; then, under hypotheses (H1)–(H5), for all t>0and all open subsetω⊂Ω,system3.9

is approximately controllable on0, t.

Proof. The proof of this theorem relies on the Criteria1and the following lemma.

Lemma 4.6. Let{α1j}j1, {β1j}j1 and {α2j}j1,{β2j}j1 be sequences of real numbers such that α11 > α12 > α13 >· · ·21 > α22 > α23 >· · · andα1j > α2j, for allj ≥0, then for any t∗ ∈R∗one

has

j1

eα1jtβ

1jeα2jtβ2j

0, ∀t∈0, t∗ ⇒β12j 0, ∀j≥1. 4.47

Proof ofLemma 4.6.By analyticity we get∞j1eα1jtβ

1jeα2jtβ2j 0, ∀t≥0 and from this we getβ11

j2eα1jα11tβ1j

j1eα2jα11tβ2j0, ∀t≥0. Under the assumptions of the lemma we get∞j2eα1jα11tβ

1jj1eα2jα11tβ2j → 0 as t → ∞and so β11 0.Ifα12 > α21, we

divide∞j2eα1jtβ 1j

j1eα2jtβ2j0 byeα12tand we passt → ∞we getβ120. Ifα21> α12,we

divide∞j2eα1jtβ

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we divide∞j2eα1jtβ

1jj1eα2jtβ2j 0 byeα12tand we passt → ∞and getβ12β21 0.But

in this we case we can integrate under the symbol of sommation over the intervall0, t and we getβ12eα21tβ21eα12t0. Henceβ12β21 0. Continuing this way we see thatβ1j β2j0, for all j≥1.

We are now ready to proveTheorem 4.5. For this purpose, we observe that

BωBω, Stw

j1

eMjtP

jw, wX, t≥0, 4.48

where{St}t0is the C0-semigroup generated by−A.

Without lose of generality, we suppose that 0< ρ1< ρ2.Hence

BωStw

j1

BωeMjtP

jw

j1

BωeMjtP

jw

j1 2

s1

BωKjteλjρstP

sj

w, 4.49

wherePsjQsPjPjQs, s1,2.

Now, suppose forwXthatBωStw0, for allt∈0, t.Then

BωStw0⇐⇒ ∞

j1 2

s1

BωKjteλjρstP

sj

wx 0, ∀x∈Ω. 4.50

If4.46is satisfied, then4.50take the form

j1 2

s1

⎛ ⎝e

λjρsλαj1c1t 0

0 eλjρsλβj2d2t

BωPsjwx 0, ∀x∈Ω. 4.51

Then, from lemma4.6we obtain that for s1,2 and allxω

BωQsPjwx Qs

⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ mj

k1

u, ϕjk

1ωϕjkx

mj

k1

v, ϕjk

ϕjkx

⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ 0 0

, j≥1. 4.52

SinceQ1Q2IR2,we get that allxω

⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ mj

k1

u, ϕjk

1ωϕjkx

mj

k1

v, ϕjk

1ωϕjkx

⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ 0 0

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On the other hand, fromTheorem 2.4we know that ϕjkare analytic functions, which implies the analticity ofEjumkj1u, ϕjkϕjkandEjvmkj1v, ϕjkϕjk.Then we can conclude that fors1,2 and allx∈Ω

⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝

mj

k1

u, ϕjk

ϕjkx

mj

k1

v, ϕjk

ϕjkx

⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠

0 0

, j≥1. 4.54

Hence Pjw 0, for all j ≥ 1, which implies that w 0. This completes the proof of

Theorem 4.5.

References

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2 H. Larez and H. Leiva, “Interior controllability of a 2×2 a reaction-diffusion system with cross diffusion matrix,” to appear inBoundary Value Problems.

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References

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